JP2000200747A - Laser device, exposure system and method using laser device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a small type ultraviolet type laser device, with which ultraviolet rays, having both sufficient output as the light source of an exposing device, etc., and low coherence, can be stably generated and a maintenance operation can be performed, and to provide an exposure system. SOLUTION: A laser beam generating part has a single wavelength oscillation laser 21, a light modulator 22 and a time-division light branching means 23, and a light-modulated pulse beam is branch-outputted to each channel of each single pulse. A light amplifier has fiber light amplifiers 24 and 25, each branched channel laser beam is amplified and outputted. The output terminal 29 of the light amplifier is formed by bundles of desired number and shape of one end of fiber. This wavelength of the bundle output is changed by a wavelength changing part and the ultraviolet ray laser of required wavelength is obtained. By the above-mentioned constitution, the diameter of the output terminal becomes 2 mm or smaller when the fiber bundle is formed in one bundle, and the wavelength changing part is composed of a pair of non-linear optical crystals.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a laser device, and more particularly to a semiconductor device, a liquid crystal display device, and an image pickup device (CCD).
And low-coherence UV light that can suppress the generation of speckles, like light sources for exposure equipment used in photolithography processes that manufacture micro devices such as thin-film magnetic heads. The present invention relates to a simple laser device and an exposure device using such a laser device.

[0002]

2. Description of the Related Art With the advancement of information equipment, semiconductor integrated circuits are required to have more functions, higher storage capacity, smaller size, and the like. For this purpose, it is necessary to increase the degree of integration of the integrated circuits. In order to increase the degree of integration, it is only necessary to reduce the size of each circuit pattern. However, the minimum pattern size of a circuit is generally determined by the performance of an exposure apparatus used in a manufacturing process.

An exposure apparatus using photolithography optically reduces and projects a circuit pattern precisely drawn on a photomask onto a semiconductor wafer coated with a photoresist and transfers the circuit pattern. The minimum pattern dimension (resolution) R on the wafer at the time of this exposure is represented by the following equation (1) according to the wavelength λ of the light source used for projection by the exposure apparatus and the numerical aperture NA of the projection optical system. It is represented by the following equation (2). R = K · λ / NA (1) DF = λ / 2 (NA) ² (2)

As is apparent from the above equation (1), in order to reduce the minimum pattern dimension R, the direction in which the constant K is reduced, the direction in which the numerical aperture NA is increased, and the wavelength λ of the light source to be projected are changed. It can be seen that there are three directions, that is, the direction of decreasing the size.

Here, the constant K is a constant determined by the projection optical system and the process, and usually takes a value of about 0.5 to 0.8. The method of reducing the constant K is called super-resolution in a broad sense. Until now, improvements in projection optical systems, modified projections, phase shift mask methods, etc. have been proposed and studied. However, there are drawbacks such as limitations on applicable patterns. On the other hand, the numerical aperture NA can be made smaller as the value of the numerical aperture NA becomes larger from the equation (1).
This also means that the depth of focus becomes shallower, as is apparent from equation (2). For this reason, there is a limit in increasing the NA value, and usually about 0.5 to 0.6 is considered appropriate in consideration of both.

Therefore, the simplest and most effective method for reducing the minimum pattern size R is to reduce the wavelength λ of light used for exposure. Here, along with the realization of a shorter wavelength, there are some conditions that must be provided for producing a light source of the exposure apparatus. Hereinafter, these conditions will be described.

First, a light output of several watts is required.
This is necessary to keep the time required for exposure and transfer of the integrated circuit pattern short.

Secondly, in the case of ultraviolet light having a wavelength of 300 nm or less, materials that can be used as lenses of the exposure apparatus are limited, and it becomes difficult to correct chromatic aberration. For this reason, the light source needs to be monochromatic, and the line width of the spectrum is required to be 1 pm or less.

Third, the temporal coherence (coherence) increases with the narrowing of the spectral line width. Therefore, if light having a narrow line width is irradiated as it is, an unnecessary interference pattern called speckle occurs. Therefore, in order to suppress the occurrence of speckle, it is necessary to reduce the spatial coherence of the light source.

Many developments have been made for shortening the wavelength of the exposure light source in order to satisfy these conditions and realize high resolution. The direction of shortening the wavelength which has been studied so far is mainly divided into the following two types. One is the development of excimer lasers whose laser oscillation wavelengths themselves are short, and the other is the development of short-wavelength exposure light sources that utilize the harmonic generation of infrared or visible light lasers. is there.

Among them, a KrF excimer laser (wavelength: 2) is used as a short wavelength light source that has been put to practical use by using the former method.
An exposure apparatus using an ArF excimer laser (wavelength: 193 nm) as a light source having a shorter wavelength is currently being developed. However, these excimer lasers are large, have high energy per pulse, and are liable to damage optical components, and use toxic fluorine gas, which makes laser maintenance complicated and expensive. There were various problems such as that.

As the latter method, there is a method of converting long-wavelength light (infrared light and visible light) into shorter-wavelength ultraviolet light by utilizing the second-order nonlinear optical effect of a nonlinear optical crystal. . For example, "Longitudinally diode pumped continuous
wave 3.5W green laser (LY Liu, M. Oka, W. Wiech
mann and S. Kubota, Optics Letters, vol. 19 (1994), p.
189) "discloses a laser light source for converting the wavelength of light from a semiconductor-excited solid-state laser. In this conventional example,
A method is described in which a 1064 nm laser beam emitted from an Nd: YAG laser is wavelength-converted using a nonlinear optical crystal to generate 266 nm light of a fourth harmonic. Note that a solid-state laser is a general term for a laser whose laser medium is solid. Therefore, in a broad sense, a semiconductor laser is also included in a solid-state laser.
d: Refers to a solid-state laser excited by light, such as a YAG laser or a ruby laser. Here, too, a distinction is made.

In an example in which a solid-state laser is used as a light source of an exposure apparatus, a laser light generating section for generating laser light;
There has been proposed an array laser in which a plurality of laser elements composed of a wavelength converter for converting the wavelength of light from the laser light generator to ultraviolet light are bundled in a matrix. For example, in Japanese Patent Application Laid-Open No. 8-334803, one laser element that generates ultraviolet light by converting light from a laser light generation unit provided with a semiconductor laser by a nonlinear optical crystal provided in a wavelength conversion unit is used. An example of an array laser which is bundled in a matrix form (for example, 10 × 10) and used as one ultraviolet light source is disclosed.

In the array laser configured as described above, by bundling a plurality of independent laser elements, it is possible to keep the optical output of each laser element low and to increase the optical output of the entire apparatus. it can. Therefore, the load on the nonlinear optical element can be reduced. However, on the other hand, since the individual laser elements are independent, when application to an exposure apparatus is considered, it is necessary to match the oscillation spectra of the entire laser element. For example, the oscillation spectral line width of each laser element is 1p
Even if it is less than m, the difference between the wavelengths of the plurality of laser elements as a whole must not be 3 pm, but must be 1 pm or less in the entire width.

For this purpose, for example, in order to cause each laser element to autonomously emit a single longitudinal mode of the same wavelength,
It was necessary to adjust the resonator length of each laser element or insert a wavelength selection element in the resonator. However, these methods have problems in that the adjustment is delicate, and that the more laser elements that constitute the method, the more complicated the structure is required to oscillate the whole at the same wavelength.

On the other hand, an injection seed method is well known as a method for actively converting a plurality of lasers into a single wavelength (for example, Solid-s by Walter Koechner).
tateLaser Engineering, 3rd Edition, Springer Serie
s in Optical Science, Vol.1, Springer-Verlag, ISBN
0-387-53756-2, p246-249). This is because the light from a single laser light source with a narrow oscillation spectrum line width is split into a plurality of laser elements, and this laser light is used as a guided wave to tune the oscillation wavelength of each laser element, and This is a method of narrowing the width. However, this method has a problem that the structure becomes complicated because an optical circuit for branching the seed light to each laser element and a tuning control unit for the oscillation wavelength are required.

Further, such an array laser can significantly reduce the size of the entire device as compared with a conventional excimer laser, but it is still difficult to reduce the output beam system of the entire array to several centimeters or less. there were. In addition, the array laser configured as described above is expensive because a wavelength conversion unit is required for each array, and is expensive when a part of the laser elements constituting the array is misaligned or when the optical element is configured. In order to adjust this laser element in case of damage to
Once the whole array is disassembled and this laser element is taken out,
There was a problem that it was necessary to reassemble the array after adjustment.

[0018]

SUMMARY OF THE INVENTION The present invention relates to the problems of the prior art described above, for example, the problem that arises when an excimer laser is used as an ultraviolet light source of an exposure apparatus. Problems, such as the use of a laser, the complexity of maintenance, and the cost, damage to a nonlinear optical crystal, and space, which can be considered when a harmonic of a solid-state laser such as an Nd: YAG laser is used as an ultraviolet light source of an exposure apparatus. Problems such as speckle generation due to an increase in dynamic coherence, and a tuning mechanism that can be considered when using an array laser in which multiple laser elements that generate ultraviolet light are bundled in a matrix as the ultraviolet light source of the exposure apparatus This is made in consideration of problems such as the complexity of the structure, the difficulty in reducing the output beam diameter, and the complexity of maintenance.

That is, an object of the present invention is to stably generate a single-wavelength ultraviolet light having a sufficiently narrow band as an ultraviolet light output having a low spatial coherence as a light source of an exposure apparatus. An object of the present invention is to provide a laser device which is compact and easy to handle. Another object of the present invention is to provide a compact and highly flexible exposure apparatus using such a small and easy-to-handle laser device as a light source.

[0020]

SUMMARY OF THE INVENTION It is an object of the present invention to provide a laser light generating section for generating light of a single wavelength, at least one stage optical amplifier having a fiber optical amplifier for amplifying the generated laser light, and the optical amplifier. And a wavelength conversion unit for converting the wavelength of the light amplified by the nonlinear optical crystal into ultraviolet light using a nonlinear optical crystal.

More specifically, the laser light generating section is provided with a narrow-band single-wavelength oscillation laser (for example, the DFB semiconductor laser 31 in the embodiment), and this single-wavelength laser light is fed to a fiber optical amplifier ( For example, erbium-doped fiber optical amplifiers 33 and 34 in the embodiment
), And output light from the fiber amplifier is converted into a nonlinear optical crystal (for example, 503 to 503 in the embodiment).
505) is converted into ultraviolet light (for example, ultraviolet light having a wavelength of 193 nm or 157 nm) by a wavelength conversion unit using a wavelength conversion unit. An object of the present invention is to provide a laser device for generating ultraviolet light having a wavelength.

In the present invention, a single-wavelength oscillation laser (for example, the DFB semiconductor lasers 11 and 2 in the embodiment) is used.
1 and a fiber laser) were branched by an optical branching means. The output was split into a plurality of outputs by the light splitting means (for example, the splitters 14 and 16 in the embodiment), fibers were provided thereafter, and the fibers were bundled to form a laser device. As the light branching means, any means may be used as long as the laser light generated by the single-frequency laser is branched into a plurality of laser beams in parallel.

Further, by providing a delay means for preventing the light from being overlapped in time, light independent from each other can be obtained. As a preferable means for this purpose, a beam splitter for splitting a plurality of laser beams generated by a single-wavelength laser into a plurality of beams in parallel is provided, and fibers having different lengths (for example, fiber 15 in the embodiment) are provided on the exit side of the beam splitter. , 17). As a preferable mode of the fibers having different lengths, for example, after the laser light branched in parallel passes through this fiber, for example, the length of each fiber is set so that the mutual delay interval is substantially constant at the fiber output end. It is to provide. In addition, as the optical branching means and the delaying means, a time division multiplexer (TD) for distributing light to each optical path at predetermined time intervals may be used.
The use of M, for example, TDM 23) in the embodiment is also one form of the present invention.

Next, as the plurality of fibers provided on the output side of the optical branching means, a plurality of fiber optical amplifiers (for example, the erbium-doped fiber optical amplifier and the yttrium-doped fiber optical amplifiers 18 and 19 in the embodiment) are used. ) Is preferably provided in, for example, two amplification stages, and the second fiber optical amplifier in the second stage is preferably configured using a large mode diameter fiber (for example, the large mode diameter fiber in the embodiment). By doing so, laser light with higher light intensity can be obtained. It is preferable to bundle a plurality of fiber optical amplifiers amplified by the fiber optical amplifier. Note that undoped fibers may be appropriately coupled to the output terminals of the plurality of fiber optical amplifiers (eg, the fiber output terminals 114 and 29 in the embodiment) as needed.

The fiber output end is provided by gradually expanding the core diameter of the fiber in a tapered shape toward the output end face (for example, the core 421 in the figure in the embodiment).
It is desirable. Further, a window member that transmits laser light (for example, the window member 43 in the embodiment) is provided at the fiber output end.
3, 443, etc.). With such a configuration, the power density (light intensity per unit area) of the laser beam at the fiber output end face can be reduced, and therefore, damage to the fiber output end can be suppressed.

According to the present invention, the output ends of the plurality of fibers provided on the incident side of the wavelength conversion unit are bundled into one or a plurality of bundles in one or more bundles according to the configuration of the wavelength conversion unit. Formed as a plurality of output groups (for example, bundle outputs 114, 2 in the embodiment)
9, 501, 601, 701, etc.).
In the wavelength converter, one or more sets of nonlinear optical crystals (for example, 502 to 50 in the fourth embodiment) are used.
4 and 842 to 844 in the fourth embodiment) to generate harmonics of the fundamental wave and to emit ultraviolet light (for example, wavelength 193n).
m or 157 nm ultraviolet light). One set of wavelength converters can be made compact and economical, and multiple sets of wavelength converters can reduce the load per set. Can be realized.

When an optical amplifier is constructed using a plurality of fiber optical amplifiers, the output light from each fiber is monitored in order to suppress variations in the ultraviolet light output due to variations in the amplification factor of each fiber amplifier. It is desirable to provide fiber output control means (for example, fiber output control means 405 and 406 in the embodiment) for controlling the excitation intensity of each fiber optical amplifier. In addition, in order to stabilize the light wavelength of the ultraviolet light output at a specific wavelength, the oscillation wavelength control means of the single wavelength oscillation laser (for example, the wavelength control in the embodiment) using the fundamental wave or the harmonic frequency in the wavelength conversion unit. Device 1274).

A light collecting optical element is provided on the incident side of the wavelength converter. The mode of use of the condensing optical element can be appropriately determined according to the output state of the optical amplifier. For example, a condensing optical element is provided for each fiber output (for example, the lenses 902 and 453 in the embodiment), Also, a condenser optical element is provided for each output group bundled in a bundle (for example, the lenses 845, 855, and 4 in the embodiment).
63 etc.) can be applied.

By the way, as a configuration for outputting ultraviolet light, for example, a laser light generating section having a wavelength of 1.5 μm is used.
m, and at least one optical amplifier having a fiber optical amplifier for amplifying a fundamental wave having a wavelength of about 1.5 μm is provided as an optical amplifier.
Further, it is composed of a wavelength converter for generating an eighth harmonic of the amplified fundamental wave. With this configuration, it is possible to generate ultraviolet light having an output wavelength near 190 nm. The output light further defines the oscillation wavelength of the laser light generator (for example, 1.544 to 1.522 μm).
m), the wavelength can be 193 nm, which is the same wavelength as the ArF excimer laser.

As another configuration for outputting ultraviolet light, for example, as in the above-described example, a laser light generator emits laser light having a wavelength of about 1.5 μm,
At least one optical amplifier having a fiber optical amplifier for amplifying a fundamental wave having a wavelength of about 1.5 μm is used as the optical amplifier.
It has a stage and is constituted by a wavelength converter for generating a tenth harmonic of the amplified fundamental wave. With this configuration, it is possible to generate ultraviolet light having an output wavelength of about 150 nm. This output light further finely defines the oscillation wavelength of the laser light generating section (for example, 1.57-1.
58 μm), the wavelength can be 157 nm which is the same wavelength as the F ₂ laser.

Further, as another configuration for outputting ultraviolet light, for example, a laser light generating section having a wavelength of 1.1 μm is used.
m, and at least one optical amplifier having a fiber optical amplifier for amplifying a fundamental wave having a wavelength of about 1.1 μm is provided as an optical amplifier.
In addition, it is composed of a wavelength conversion unit that generates a seventh harmonic of the amplified fundamental wave. With this configuration, it is possible to generate ultraviolet light having an output wavelength of about 150 nm.
The output light is 157 nm which is the same wavelength as that of the F ₂ laser by further defining the oscillation wavelength of the laser light generation unit (for example, 1.099 to 1.106 μm).
It can be.

Other configurations for outputting ultraviolet light include, for example, a laser light generator having a semiconductor laser or fiber laser having an oscillation wavelength of around 990 nm, and a fiber amplifier for amplifying a fundamental wave having a wavelength of around 990 nm. By having at least one stage of an optical amplifier and a wavelength converter for generating a fourth harmonic of the amplified fundamental wave, it is possible to obtain ultraviolet light having a wavelength of 248 nm, which is the same as that of a KrF excimer laser. It is possible.

The configuration of the wavelength converter for generating such harmonics can take various configurations as described in detail in the embodiments. For example, a configuration example of a wavelength conversion unit that generates an eighth harmonic of a fundamental wave will be briefly described. If a second harmonic generation (SHG) of a nonlinear optical crystal is used for all wavelength conversion stages, a fundamental wave is generated. → 2nd harmonic → 4
It can be constituted by a three-stage harmonic generation optical path system (for example, FIG. 11A in the fourth embodiment) in which the harmonic is changed to the eighth harmonic. With this configuration, a desired eighth harmonic can be obtained with the minimum number of stages.

Another preferable configuration for obtaining the 8th harmonic is to use the sum frequency generation (SFG) of the nonlinear optical crystal in combination with the wavelength conversion stage to obtain the third harmonic of the fundamental wave and the 4th harmonic. A configuration in which harmonics are generated, and these are generated at the 7th harmonic of the fundamental wave by sum frequency generation, and the 7th harmonic and the fundamental wave are generated at the 8th harmonic of the fundamental wave by sum frequency generation. (For example, FIG. 11D in the fourth embodiment)
etc). This configuration is 193 nm for the eighth harmonic generation in the final stage.
LBO crystal having a low absorption coefficient of ultraviolet light can be used. The 7th harmonic generation and the 10th harmonic generation of the fundamental wave are appropriately configured by using the second harmonic generation and the sum frequency generation of the nonlinear optical crystal as in the case of the 8th harmonic generation of the fundamental wave. be able to.

Further, in the laser device of the present invention, the light from the light source (for example, the DFB semiconductor laser 11 in the embodiment) that generates continuous light is converted into the pulse light by the optical modulator (for example, the light in the embodiment). Modulating elements 12, 22
Or the like, or by oscillating a single-wavelength oscillation laser with a pulse, an ultraviolet pulsed laser beam can be obtained.

Then, the laser device obtained as described above is used as a light source of a projection exposure apparatus, and a mask (for example, a reticle 1263 in the embodiment) on which a pattern to be projected is drawn from the light source with almost uniform intensity. An illumination optical system (for example, the illumination optical system 1262 according to the embodiment) for irradiating the light, and a projection objective optical system (for example, the projection optical system 1265 according to the embodiment) for projecting the pattern drawn on the mask onto the wafer. By having
A projection exposure apparatus with easy maintenance can be obtained.

Further, a part of the fiber output amplified by the plurality of fiber optical amplifiers is divided (for example, the fiber bundle output 850 in the embodiment), and the first fiber transmission system (for example, the fiber bundle output to the illumination optical system of the exposure apparatus) is divided. An alignment system that is connected to a second fiber transmission system (for example, the connection fiber 1278 in the embodiment) different from the connection fiber 1273 in the embodiment and detects an alignment mark formed on a mask or a reference mark on a wafer stage. Constituting (for example, the alignment systems 1280 and 1281 in the embodiment) is a preferred embodiment of the exposure apparatus using the laser apparatus of the present invention.

[0038]

BEST MODE FOR CARRYING OUT THE INVENTION A laser light source according to the present invention amplifies light of a single wavelength from a laser light generator by an optical amplifier, and converts the amplified light into ultraviolet light by a nonlinear optical crystal provided in a wavelength converter. With the configuration for conversion, ultraviolet light having a required spectral line width (for example, 1 pm or less) can be easily obtained without using a complicated configuration.

Further, the laser light of a single wavelength is divided into a plurality (or time-divided), the output light is amplified by a plurality of fiber optical amplifiers, and the amplified light is converted into ultraviolet light by a nonlinear optical crystal. With this configuration, it is intended to increase the laser light output of the entire light source while suppressing the peak power per pulse of the pulse light, and to supply ultraviolet light having low spatial coherence of light.

Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings. First, a first embodiment of a laser device according to the present invention will be described with reference to FIG. The ultraviolet light generation device according to the present embodiment includes a laser light generation unit that includes a single wavelength oscillation laser 11 and generates a single wavelength laser light, and fiber optical amplifiers 13 and 1.
8 and 19, an optical amplifier for amplifying the light, optical splitting means 14 and 16 for splitting the light into a plurality of lights in parallel, fibers 15 and 17 having different lengths, and a non-linear optical crystal described later. And a wavelength converter that converts the wavelength of the converted light into a wavelength, and generates the same output wavelength (193 nm) as the ArF excimer laser or the same output wavelength (157 nm) as the F ₂ laser, and has a low spatial coherence. Is what you do.

In this embodiment, FIG. 1 shows an example of a configuration of a laser device according to the present invention until a single-wavelength laser beam output from a laser beam generator is branched and amplified.
First, referring to FIG. 1, the laser light generating section includes a single-wavelength oscillation laser 11 that generates a single-wavelength laser light, and further includes splitters 14 and 16 that are optical branching means. Fibers 15 and 17 of different lengths
Fiber optical amplifiers 18 and 19 are connected to the emission sides of fibers 17 having different lengths, and a plurality of fiber optical amplifiers are amplified in parallel.

The output end of the fiber optical amplifier 19 is bundled in a bundle, and the amplified laser light is incident on, for example, a wavelength converter (502 to 506) shown in FIG. The fiber bundle output end 114 of the fiber optical amplifier 19 shown in FIG.
The output end 5 of the fiber bundle shown in FIG.
Corresponds to 01. This wavelength conversion section includes the nonlinear optical crystal 5
It converts the fundamental wave emitted from the fiber optical amplifier 19 into ultraviolet light. In addition,
The wavelength converter according to the present invention will be described in detail as Embodiments 4 to 7 later in the embodiment of the present invention.

Hereinafter, the present embodiment will be described in more detail. As the single wavelength oscillation laser 11 oscillating at a single wavelength shown in FIG. 1, for example, InGaAsP having an oscillation wavelength of 1.544 μm and a continuous wave output (hereinafter referred to as CW output) of 20 mW,
A DFB semiconductor laser is used. Here, a DFB semiconductor laser is a device in which a diffraction grating is formed in a semiconductor laser in place of a Fabry-Perot resonator having low longitudinal mode selectivity. Distributed feedback type (Distributed
Feedback: DFB) laser. Since such a laser basically oscillates in a single longitudinal mode, its oscillation spectrum line width can be suppressed to 0.01 pm or less.

In order to fix the output wavelength of the laser device to a specific wavelength, a single-wavelength oscillation laser (Master Oscill
ator) is preferably provided with an oscillation wavelength control device for controlling the oscillation wavelength to a constant wavelength. Conversely, it is preferable that the oscillation wavelength of the single-wavelength oscillation laser is positively changed by the oscillation wavelength control device so that the output wavelength thereof can be adjusted. For example, when the laser apparatus of the present invention is applied to an exposure apparatus, according to the former, the generation or aberration of the projection optical system due to wavelength fluctuation is prevented, and its image characteristics (such as image quality) during pattern transfer are prevented. Optical characteristics) do not change.

According to the latter, an altitude difference and a pressure difference between a manufacturing site where the exposure apparatus is assembled and adjusted and a place where the exposure apparatus is installed (delivery destination), a difference in environment (atmosphere in a clean room), and the like. Therefore, fluctuations in the imaging characteristics (such as aberration) of the projection optical system caused by the deviation can be offset, and the time required for starting up the exposure apparatus at the delivery destination can be reduced. Furthermore, according to the latter, during the operation of the exposure apparatus, the irradiation of the exposure illumination light, and the aberration of the projection optical system caused by a change in the atmospheric pressure, the projection magnification, and the fluctuation of the focal position, etc. can be canceled out, and it is always possible to cancel. The pattern image can be transferred onto the substrate in the best image forming state.

For example, when a DFB semiconductor laser is used as a single-wavelength oscillation laser, such oscillation wavelength control means can be achieved by controlling the temperature of the DFB semiconductor laser. The wavelength can be further stabilized to control the wavelength to be constant, or the output wavelength can be finely adjusted.

Normally, a DFB semiconductor laser or the like is provided on a heat sink, and these are housed in a housing. Therefore, in this example, the oscillation wavelength is adjusted by controlling the temperature using a temperature controller (for example, a Peltier element or the like) provided on a heat sink attached to the single-wavelength oscillation laser (such as a DFB semiconductor laser) 11. Where DFB
In a semiconductor laser or the like, the temperature can be controlled in units of 0.001 ° C.

The oscillation wavelength of the DFB semiconductor laser has a temperature dependency of about 0.1 nm / ° C. For example, DF
When the temperature of the B semiconductor laser is changed by 1 ° C., the fundamental wave (1
544 nm), the wavelength changes by 0.1 nm.
In the eighth harmonic (193 nm), the wavelength is 0.0125 nm.
And at the 10th harmonic (157 nm), the wavelength is 0.0
It will change by 1 nm. In the exposure apparatus, the wavelength of the exposure illumination light (pulse light) is set to ± 2 with respect to the center wavelength.
It is sufficient if it can be changed by about 0 pm. Therefore, the temperature of the DFB semiconductor laser 11 is ± 1.
It may be changed by about ± 2 ° C. for about 6 ° C. and 10th harmonic.

As the monitor wavelength for feedback control when controlling the oscillation wavelength to a predetermined wavelength,
From the oscillation wavelength of the DFB semiconductor laser or the wavelength conversion output (2nd harmonic, 3rd harmonic, 4th harmonic, etc.) described below, the wavelength that gives the sensitivity necessary for performing the desired wavelength control and is the most easily monitored wavelength select. For example, as a single-wavelength oscillation laser, D with an oscillation wavelength of 1.51 to 1.59 μm
When an FB semiconductor laser is used, the third harmonic of the oscillation laser light has a wavelength of 503 nm to 530 nm, and this wavelength band corresponds to a wavelength range where absorption lines of iodine molecules are densely present. Precise oscillation wavelength control can be performed by selecting an appropriate absorption line of the molecule and locking the wavelength.

The light output of the semiconductor laser is applied to an optical modulator 1 such as an electro-optical modulator or an acousto-optical modulator.
2 is used to convert CW light (continuous light) into pulsed light.
In the present configuration example, as an example, a case where the light modulation element 12 modulates the pulse light into a pulse light having a pulse width of 1 ns and a repetition frequency of 100 kHz (pulse period of 10 μs) will be described. As a result of performing such light modulation, the light modulation element 1
2 has a peak output of 20 mW and an average output of 2 μW. Here, it is assumed that there is no loss due to the insertion of the optical modulation element 12. However, when the insertion loss is present, for example, when the loss is −3 dB, the peak output of the pulse light is 10 mW and the average output is 1 μW.

When an electro-optic modulator is used as the light modulator, an electrode having a chirp-corrected electrode structure such that the wavelength spread of the semiconductor laser output due to the chirp due to the change in refractive index with time is reduced. It is preferable to use an optical modulation element (for example, a two-electrode modulator). Further, by setting the repetition frequency to about 100 kHz or more, it is possible to prevent a decrease in amplification factor due to the influence of ASE (Amplified Spontaneous Emission) noise in a fiber optical amplifier described later. It is desirable that

In a semiconductor laser or the like, the output light can be pulse-oscillated by controlling the current. For this reason, in this example (and each embodiment described later), it is preferable to generate pulsed light by using both the current control of the single-wavelength oscillation laser (such as a DFB semiconductor laser) 11 and the light modulation element 12. Therefore, by controlling the current of the DFB semiconductor laser 11, a pulse light having a pulse width of, for example, about 10 to 20 ns is oscillated, and only a part of the pulse light is cut out from the pulse light by the light modulation element 12, that is, in this example, the pulse width is Modulates into 1 ns pulsed light.

As a result, compared with the case where only the light modulation element 12 is used, it is possible to easily generate a pulse light having a narrow pulse width, and it is also possible to determine the oscillation interval of the pulse light and the start and stop of the oscillation. Control becomes easier. In particular, when the extinction ratio is not sufficient even when the pulse light is turned off using only the light modulation element 12, it is desirable to use the current control of the DFB semiconductor laser 11 together.

The pulsed light output thus obtained is connected to an erbium (Er) -doped fiber optical amplifier (EDFA) 13 at the first stage, and a light amplification of 35 dB (3162 times) is performed. At this time, the pulse light has a peak output of about 63
W, the average output is about 6.3 mW.

The output of the fiber amplifier 13 which is the first-stage optical amplifier is first divided by a splitter 14 (a flat waveguide 1 × 4 splitter) which is an optical branching means into channels 4 to 3 of channels 0 to 3.
Split into parallel outputs. Each output of channels 0 to 3 is
By connecting to fibers 15 having different lengths (only one channel 0 is shown in the figure), each light output from each fiber is given a delay corresponding to the fiber length. For example, in the present embodiment, it is assumed that the propagation speed of light in the fiber is 2 × 10 ⁸ m / s, and the channels 0, 1, 2, and 3 are 0.1 m and 1 m respectively.
Connect fibers of 9.3m, 38.5m, 57.7m length. In this case, the light delay between adjacent channels at each fiber exit is 96 ns. Here, the fiber used for the purpose of delaying light in this way is called a delay fiber for convenience.

Next, the output of the four delay fibers is
The block is further divided into 32 outputs in parallel by 4 blocks of a flat waveguide 1 × 32 splitter 16 (channels 0 to 3 in each block).
1) Divide into 128 channels in total. Then, the delay fibers 17 having different lengths are connected again to the channels 1 to 31 except the channel 0 in each block. For example, in this embodiment, channels 1 to 31 each have 0.6
A fiber having a length of × N meters (N is a channel number) is connected. As a result, a delay of 3 ns is given between adjacent channels in each block, and the output of channel 31 is 3 × 31 = 93 with respect to the output of channel 0 of each block.
An ns delay is provided.

On the other hand, a delay of 96 ns is given between the first to fourth blocks by the delay fiber 15 at the time of input of each block as described above. Accordingly, the channel 0 output of the second block has a delay of 96 ns with respect to the channel 0 output of the first block, and the delay with the channel 31 of the first block is 3 ns. This is the same between the second and third blocks and the third and fourth blocks. As a result, a total output of 12
At the output terminals of the eight channels, pulse light having a delay of 3 ns between adjacent channels is obtained. In FIG. 1, only the channel 1 of the first block is described, and the description of other channels is omitted. However, other channels are similarly configured.

By the above-described branching and delay, pulse light having a delay of 3 ns between adjacent channels is obtained at the output terminals of a total of 128 channels. At this time, the optical pulse observed at each output terminal is an optical pulse. The same 100 kHz as the pulse modulated by the modulation element 12 (pulse period 10 μm)
s). Therefore, looking at the entire laser beam generator, 9.62 after generating 128 pulses at 3 ns intervals.
The repetition that the next pulse train is generated at intervals of μs is performed at 100 kHz. That is, the total output is 12
8 × 100 × 10 ³ = 1.28 × 10 ⁷ pulses / sec.

In this embodiment, an example has been described in which the number of divisions is set to 128 and a short delay fiber is used. For this reason, 9.62 μ between each pulse train.
Although an interval where s does not emit light occurs, the number of divisions is increased,
Or by using a longer delay fiber to an appropriate length, or by using a combination of these,
It is also possible to make the pulse intervals completely equal. For example, when the number of pulse repetitions of the laser beam incident on the splitter 14 is f [Hz] and the number of divisions is m, the length of each fiber is set so that the delay interval of each fiber is 1 / (f × m). It can also be achieved by setting.

Further, the number of divisions of at least one of the splitters 14 and 16 or the number of pulse repetitions f defined by the light modulation element 12 is adjusted so that the above-mentioned pulse intervals are completely equal, or the division is made. Both the number and the number of repetitions f may be adjusted. Therefore, each fiber length of the delay fibers 15 and 17 and the splitter 1
By adjusting at least one of the number of divisions 4 and 16 and the number of pulse repetitions f, not only pulse intervals can be set at equal intervals, but also the intervals can be set arbitrarily.

In order to change the fiber length after assembling the light source, for example, the delay fibers 15 and 17 are required.
Are preferably bundled into a unit so that this unit can be replaced with another delay fiber unit having a different delay time between channels. Also, when changing the number of divisions of the splitters 14 and 16, it is preferable to prepare another splitter having a different number of divisions corresponding to each of the splitters 14 and 16 and to replace them. At this time, it is desirable that the units of the delay fibers 15 and 17 be exchangeable in accordance with the change in the number of divisions of the splitters 14 and 16.

In this embodiment, the oscillation timing of the light source (pulse light), that is, the repetition frequency f (pulse cycle) can be adjusted by controlling the timing of the drive voltage pulse applied to the light modulation element 12. . Further, when the output of the pulse light can fluctuate with the change of the oscillation timing, the magnitude of the driving voltage pulse applied to the light modulation element 12 is also adjusted at the same time to compensate for the output fluctuation. Good.

At this time, the output fluctuation of the pulsed light may be compensated by only controlling the oscillation of the single-wavelength oscillation laser 11 or by using the control of the light modulation element 12 described above. Note that the output fluctuation of the pulse light is caused not only when the oscillation timing is changed, but also when the output of the single-wavelength oscillation laser (that is, the pulse light enters the fiber optical amplifier).
May occur when the oscillation is restarted after stopping the operation for a predetermined time. When the single-wavelength oscillation laser 11 is pulse-oscillated, the oscillation timing (pulse cycle) of the pulsed light is adjusted only by controlling the current of the single-wavelength oscillation laser 11 or in combination with the control of the light modulation element 12 described above. You may do it.

In this example, a fiber optical amplifier 18 is connected to each of the 128 delay fibers 17, and a fiber optical amplifier 19 is connected with a narrow band filter 113 interposed therebetween. The narrow band filter 113 is provided with the ASE generated by the fiber optical amplifiers 13 and 18, respectively.
By cutting the light and transmitting the output wavelength of the DFB semiconductor laser 11 (the wavelength width is about 1 pm or less), the wavelength width of the transmitted light is substantially narrowed. As a result, the ASE light is transmitted to the subsequent fiber optical amplifier (18 and 1).
9), it is possible to prevent the amplification gain of the laser beam from being lowered by entering. Here, the narrow band filter preferably has a transmission wavelength width of about 1 pm.
Since the wavelength width of the light is about several tens of nm, the ASE light can be cut to such an extent that there is no practical problem even if a narrow band filter whose transmission wavelength width obtained at the present time is about 100 pm is used.

When the output wavelength of the DFB semiconductor laser 11 is positively changed, the narrow band filter may be replaced in accordance with the output wavelength. ± 20p
m) is preferably used. In a laser device applied to an exposure apparatus, the wavelength width is set to about 1 pm or less. In addition, the laser device of FIG. 1 is provided with three isolators 110, 111, and 112, which reduce the influence of return light.

With the above configuration, the output light from the generating section (the output end of the fiber optical amplifier 19) does not overlap with each other in time while being extremely narrow band light. . Therefore, spatial coherence between channel outputs can be reduced.

In the above configuration, an example has been described in which a DFB semiconductor laser is used as the single-wavelength oscillation laser 11 and the planar waveguide type splitters 14 and 16 are used as branching elements of the optical branching means. , DFB
As with the semiconductor laser, any laser having a narrow band in this wavelength region may be used. For example, an erbium (Er) -doped fiber laser can provide the same effect. Further, as the branching element of the light branching means, as in the case of the flat-plate waveguide splitter, any element may be used as long as it splits light in parallel. It works.

As described above, in the present embodiment, the output of the fiber 17 which is a delay fiber is further amplified by a single-stage or multi-stage EDFA (erbium-doped fiber optical amplifier, hereinafter the same). In this embodiment, as an example, an average output of about 50 μW for each channel in the laser light generating section and an average output of about 6.3 mW for the total of all channels are output by the two-stage EDFAs 18 and 19 for a total of 4 m.
An example in which amplification of 6 dB (40600 times) is performed is shown. In this case, the peak output is 2 at the output end of each channel.
0 kW, pulse width 1 ns, pulse repetition 100 kW
z, average power 2W, average power about 256W in all channels
Get.

Here, the planar waveguide type splitter 14,
Although the coupling loss at 16 is not taken into account, if there is such coupling loss, it is generated from the EDFA 19 by increasing the amplification gain of the fiber optical amplifier (for example, at least one of the EDFAs 18 and 19) by the loss. The output of the fundamental wave can be made the same as the above-described value (for example, the peak output is 20 kW). By changing the amplification gain of the fiber optical amplifier, the output of the fundamental wave can be made larger or smaller than the above-described value.

The wavelength 1.544, which is the output of this optical amplifier,
The μm single-wavelength pulse laser light is converted into an ultraviolet light pulse output having a narrow spectral line width by a wavelength conversion unit using a nonlinear optical crystal. An embodiment of the wavelength converter will be described later.

Next, a second embodiment of the laser device according to the present invention will be described with reference to FIG. The ultraviolet light generation device according to the present embodiment includes a laser light generation unit that generates a single-wavelength laser light, an optical amplifier that amplifies the light, and a wavelength conversion unit that wavelength-converts the amplified light. , The same output wavelength as the ArF excimer laser (193n
m) or the same output wavelength as the F ₂ laser (157 nm)
The present invention provides an ultraviolet laser device that generates a laser beam and has low spatial coherence. The first of the present invention
The ultraviolet laser device according to the embodiment is characterized in that the light splitting means splits and splits the light in time, and that the laser light until entering the light splitting means is not amplified by the fiber optical amplifier. , In two respects.
Of these, any configuration is possible before and after the optical branching means and the fiber optical amplifier.

Further, similarly to the first embodiment (FIG. 1), a fiber optical amplifier is further provided on the incident side (single wavelength oscillation laser 21 side) of the optical branching means (TDM 23 in this example), and the amplification is performed here. The pulsed light may be configured to be incident on the optical branching unit. Thus, the fiber optical amplifier (24, in this example) disposed downstream of the optical branching means.
In 25), the required amplification gain can be reduced as compared with the configuration of FIG. 2, and the number of replacements of the fiber optical amplifier is reduced, which is more economical.

By the way, in this embodiment, FIG. 2 shows an example of the configuration of the laser beam generating section, the optical branching means, and the optical amplifier of the ultraviolet laser device according to the present invention. As shown in FIG. 2, the ultraviolet laser device according to the present embodiment includes a laser light generation unit including a single-wavelength oscillation laser 21 that generates a single-wavelength laser light, and a light branching unit 23 that branches light. A plurality of optical outputs from the optical branching means 23 are amplified in parallel by fiber optical amplifiers 24 and 25, respectively. The emission end of the fiber optical amplifier 25 is bundled in a bundle, and the amplified laser light is incident on a wavelength converter (702 to 712) made of, for example, a nonlinear optical crystal shown in FIG.

The fiber bundle output end 29 of the fiber optical amplifier 25 shown in FIG. 2 corresponds to the fiber bundle output end 701 shown in FIG.
The wavelength conversion unit includes a group of nonlinear optical crystals 702, 70
5, 710, 712, and an optical amplifier (21
To 28) are converted into ultraviolet light. The wavelength conversion unit according to the present invention will be described in detail as Embodiments 4 to 7 later in the embodiment.

Hereinafter, the present embodiment will be described in more detail. The laser 21 oscillating at a single wavelength shown in FIG. 2 has, for example, an oscillation wavelength of 1.099 μm and a CW output of 20 m.
W DFB semiconductor laser or yttrium (Y
b) Use a doped fiber laser. Since these lasers basically oscillate in a single longitudinal mode, their oscillation spectral line width can be suppressed to 0.01 pm or less.

The light output of the semiconductor laser is applied to an optical modulator 2 such as an electro-optical modulator or an acousto-optical modulator.
2 is used to convert CW light (continuous light) into pulsed light.
In the present configuration example, as an example, a case will be described in which the light modulation element 22 modulates the pulse light into a pulse light having a pulse width of 1 ns and a repetition frequency of 12.8 MHz (pulse cycle of about 78 ns). As a result of performing such light modulation, the peak output of the pulse light output from the light modulation element is 20 mW, and the average output is 0.256 mW.

This pulsed light output is converted into a time division multiplexer (TDM) as an optical branching means.
23, the pulse light is sequentially distributed to a total of 128 channels of channel 0 to channel 127 for each pulse. That is, the pulses of every pulse cycle of 78 ns are sequentially distributed from channel 0 to channels 1, 2, 3,... Looking at this result for each channel, the pulse period of the output pulse is 78 ns × 128 = 1.
The pulse light has 0 μs (pulse frequency 100 kHz), a pulse peak output of 20 mW, and an average output of 2 μW. Also,
Looking at the entire laser beam generator, the pulse frequency is 12.8M
Hz, pulse peak output 20 mW, average output 0.256
It becomes an averaged pulse light of mW. Note that there is a 78 ns delay between adjacent channels, and the pulsed light between the channels does not overlap each other.

In this embodiment, the repetition frequency f of the pulse light output from the light modulation element 22 is set to 100 kHz (pulse cycle is 10 μs), and the time division optical branching means (TDM)
Pulse light output from 23 channels 0 to 127 is
The pulse period defined by the light modulation element 22 (10 μm)
Although s) is delayed by a time interval (78 ns) obtained by equally dividing 128, the delay time may not be an equal time interval, or the pulse period (10 μs) may be the same as in the first embodiment. Channel 0 to 12
7 may output pulse light. Further, the timing of the drive voltage pulse applied to the light modulation element 22 is simultaneously controlled to control the pulse cycle (10 μm).
s) may be changed. For example, the delay time which is a time interval obtained by dividing the changed pulse cycle into 128 equal parts may be changed.

Incidentally, similarly to the above-described first embodiment,
Also in this example, the single-wavelength oscillation laser 21 may be pulse-oscillated. Further, the pulse period (10 μs) may be changed by using the time division optical branching device (TDM) 23 and the current control of the single wavelength oscillation laser 21 together or by further using the control of the light modulation element 22. good.

With the above-described configuration, the output light from the generating unit does not overlap with each other in time, although it is light of a single wavelength having a very narrow band. Therefore, spatial coherence between channel outputs can be reduced.

In the above configuration, the DFB semiconductor laser or the ytterbium laser is used as the single-wavelength oscillation laser 21.
Although an example using a (Yb) -doped fiber laser has been described, a laser light source having a narrow band in this wavelength region has the same effect as a DFB semiconductor laser.

The output of the time-division optical branching means 23 is a fiber optical amplifier composed of a single-stage or multi-stage YDFA (yttrium-doped fiber optical amplifier, hereinafter the same) provided for the channels 0 to 127, respectively. Amplified by 24, 25. The ytterbium-doped fiber optical amplifier has a higher pumping efficiency by a semiconductor laser than the erbium-doped fiber optical amplifier described above, and is economical. In addition, similarly to the first embodiment (FIG. 1), the single-wavelength oscillation laser 21 is used for the purpose of reducing the influence of the return light and narrowing the wavelength width.
An isolator 26 is arranged between the optical modulator 22 and the optical modulator 22, and a narrow band filter 28 and an isolator 27 are arranged between the fiber optical amplifiers 24 and 25.

In the present embodiment, as an example, the average output of each channel of the time-division optical branching means 23 is 2 μW, and the average output of all the channels is 0.256 mW.
25 shows an example of performing amplification of a total of 60 dB (1,000,000 times). In this case, at the output end of each channel, a peak output of 20 kW, a pulse width of 1 ns, a pulse repetition of 100 kHz, an average output of 2 W, and an average output of 256 W for all channels are obtained. Although FIG. 3 shows only channel 0 among all channels and omits the description of other channels, other channels are similarly configured.

The wavelength of 1.099 which is the output of this optical amplifier
The μm single-wavelength pulse laser light is converted into an ultraviolet light pulse output having a narrow spectral line width by a wavelength conversion unit using a nonlinear optical crystal. An embodiment of the wavelength converter will be described later.

Although the output wavelengths of the optical amplifiers are different between the first and second embodiments described above, these are different from the single-wavelength oscillating lasers (11, 2
A fiber optical amplifier determined by the oscillation wavelength of 1) and further considering the amplification efficiency, that is, a gain wavelength width (for example, 1530 to 1560 n in the case of erbium-doped fiber)
m, 990 for ytterbium-doped fiber
1200 nm). Therefore, in the embodiment of the present invention, a fiber optical amplifier having a gain wavelength width corresponding to the oscillation wavelength may be appropriately selected and combined with the single wavelength oscillation laser. Further, for example, in the first embodiment, the TDM used in the second embodiment is used instead of the planar waveguide splitter (14, 16).
(23) may be used. In the second embodiment, TDM (2
Instead of 3), a flat-plate waveguide type splitter may be used. An embodiment of the wavelength converter will be described later.

The last stage high peak output fiber optical amplifier (19 in FIG. 1, FIG.
In 25), in order to avoid an increase in the spectrum width of the amplified light due to the non-linear effect in the fiber, the fiber mode diameter is usually used in communication (5 to 6).
It is desirable to use a large mode diameter fiber optical amplifier wider than [mu] m, for example 20-30 [mu] m.

FIG. 4 shows a configuration example of an optical amplifier using this large mode diameter fiber optical amplifier. In this optical amplifier 42 in which the portion of the fiber enclosed by the dotted rectangle in FIG. 4 has a wide mode diameter, the semiconductor laser 4 for exciting the optical amplifier doped fiber having the wide mode diameter is used.
3 is coupled to a large mode diameter fiber corresponding to the diameter of a doped fiber for an optical amplifier, and the output of this semiconductor laser is wavelength-division multiplexed (Wavelength Division Multiplexer).
Multiplexer (WDM) 45 and 46 are used to input the doped fiber for the optical amplifier to excite the doped fiber.

This large mode diameter fiber (optical amplifier) 4
The laser light amplified in step 2 enters the wavelength converter 500,
Here, the wavelength is converted to ultraviolet laser light. Laser light (signal) to be amplified that propagates through this large mode diameter fiber
Is preferably mainly a fundamental mode, which can be realized in a single mode or a multimode fiber having a low mode order by mainly selectively exciting the fundamental mode.

In FIG. 4, the semiconductor laser 43 and W
An optical polarization coupling element 44 is provided between the laser diode and the DM 45 so that laser beams output from the two semiconductor lasers 43 whose polarization directions are orthogonal to each other can be combined. In this example, the polarization directions of the laser beams are orthogonalized by the optical polarization coupling element 44. However, the polarization directions need not be orthogonalized if a reduction in the efficiency of combining laser beams can be tolerated. Further, the influence of the return light is reduced by the isolator 404 provided on the incident side of the large mode fiber optical amplifier 42.

Further, a narrow band filter 403 is provided between the fiber optical amplifier 41 having a standard mode diameter and the large mode diameter fiber optical amplifier 42 in order to remove ASE light generated from the fiber optical amplifier 42. ing. A semiconductor laser 401 for excitation is fiber-coupled to the fiber optical amplifier 41, and the output of the semiconductor laser 401 is input to the doped fiber for optical amplifier through the WDM 402, whereby the doped fiber is excited. You.

According to such a method, since the semiconductor laser 43 is coupled to the large mode diameter fiber, the coupling efficiency to the fiber is improved, and the output of the semiconductor laser can be used effectively. Further, by using a large mode diameter fiber having the same diameter, WDM45,
It is efficient because the loss at 46 can be reduced. In addition, the fiber optical amplifier 41 of the previous stage having a standard mode diameter
And the last stage fiber optical amplifier 4 having a wide mode diameter.
The connection with 2 is performed using a fiber whose mode diameter increases in a tapered shape.

Further, the final stage fiber optical amplifier (1)
In order to obtain a high output in 9 and 25), a double clad fiber 410 having a double fiber clad structure may be used instead of the large mode diameter fiber (42) in FIG. . One example of a cross-sectional view of the fiber 410 is shown in FIG. In this structure,
The core 411 is doped with ions that contribute to the amplification of the laser light, and the amplified laser light (signal) propagates through the core. First cladding 412 surrounding core
Is coupled with a semiconductor laser for excitation. The first cladding is multi-mode and has a large cross-sectional area, so that high-power excitation semiconductor laser light can be easily transmitted, and efficiently couples a multi-mode oscillation semiconductor laser.
The excitation light source can be used efficiently. A second clad 413 for forming a waveguide of the first clad is formed on the outer periphery of the first clad.

In addition, a quartz fiber or a silicate fiber can be used as the fiber optical amplifier in the first and second embodiments. In addition, a fluoride fiber such as a ZBLAN fiber is used. You may. In this fluoride-based fiber, the erbium doping concentration can be increased as compared with quartz or silicate-based fibers, so that the fiber length required for amplification can be shortened.

This fluoride fiber is preferably applied to the fiber optical amplifiers (19, 25) at the final stage, and by shortening the fiber length, the spread of the wavelength width due to the non-linear effect during the propagation of the pulsed light into the fiber is reduced. For example, it is possible to obtain a light source in which the wavelength width required for the exposure apparatus is narrowed. In particular, the fact that the band narrowing light source can be used in an exposure apparatus having a projection optical system having a large numerical aperture is advantageous in designing and manufacturing a projection optical system, for example.

By the way, as described above, the output wavelength of the fiber optical amplifier having the cladding having the double structure is 1.51.
When using a thickness of ~ 1.59 µm, it is preferable to dope yttrium together with erbium as ions to be doped. This is because there is an effect of improving the pumping efficiency by the semiconductor laser. That is, when doping both erbium and yttrium, the strong absorption wavelength of yttrium extends around 915 to 975 nm, and a plurality of semiconductor lasers having different oscillation wavelengths at wavelengths near this are coupled by WDM to form the first semiconductor laser. By coupling to the cladding, the plurality of semiconductor lasers can be used as excitation light, so that a large excitation intensity can be realized. Further, for example, if a polarization coupling element is used as the optical coupling element 44 in FIG. 4, the outputs of the semiconductor lasers having different polarization directions can be coupled together, so that the excitation intensity can be further doubled.

As for the design of a doped fiber of a fiber optical amplifier, an apparatus (for example, an exposure apparatus) that operates at a predetermined fixed wavelength as in the present invention.
Then, the material is selected so that the gain of the fiber optical amplifier at a desired wavelength is increased. For example, in an ultraviolet laser device for obtaining the same output wavelength (193 to 194 nm) as an ArF excimer laser, a desired wavelength, for example, 1.548 μm is used when an optical amplifier fiber is used.
It is desirable to select a material that increases the gain at the time.

However, the communication fiber is designed to have a relatively flat gain in a wavelength region of several tens nm near 1.55 μm for wavelength division multiplexing communication. Therefore, for example, in a communication fiber having an erbium single-doped core as an excitation medium, a method of co-doping aluminum or phosphorus into a silica fiber is used to realize the flat gain characteristic. Therefore, in this type of fiber, the gain does not always increase at 1.548 μm. This is shown in FIG.

FIG. 6 shows the difference in the fluorescence intensity characteristics between the fibers by taking the wavelength on the horizontal axis and the fluorescence intensity on the vertical axis. Al / P Silica in the figure corresponds to the cable material for communication. On the other hand, if Silicate L22 shown in FIG. 6 is used, a higher gain can be obtained at 1.547 μm. Further, aluminum as a doping element has an effect of shifting a peak around 1.55 μm to a longer wavelength side, and phosphorus has an effect of shifting to a shorter wavelength side. Therefore, the gain can be increased near 1.547 μm by doping a small amount of phosphorus into the silicate L22.

On the other hand, when an optical amplifier fiber (for example, the double clad type fiber) having a core doped (co-doped) with both erbium and ytterbium is used, as shown in FIG. By adding a small amount of phosphorus to, a higher gain can be obtained around 1.547 μm. FIG. 7 shows the change in gain with respect to wavelength when the abscissa indicates wavelength and the ordinate indicates gain per unit length. In the figure, the excitation intensity is changed and the population inversion density is changed. It is.

In the fiber optical amplifiers according to the first and second embodiments, since each fiber is an independent optical amplifier, the difference between the gains of the optical amplifiers causes variations in the optical output of each channel. Therefore, in the laser device of such a form, as shown in FIG. 8, for example, a part of the output is branched by the fiber optical amplifiers (41, 42) of the respective channels to monitor the light intensity, and the respective fiber optical amplifiers are monitored. The pumping semiconductor lasers (401, 4
It is desirable to provide fiber output control devices 405 and 406 that feedback-control the drive current of 3). In FIG. 8, a fiber output control device 405 for detecting the branch light from the fiber optical amplifier 41 controls the drive current of the semiconductor laser 401 connected to the fiber optical amplifier 41 based on the detected value, and A fiber output control device 406 for detecting the branched light from the optical amplifier 42 has a semiconductor laser 4 connected to the large mode fiber optical amplifier 42 based on the detected value.
3 is controlled.

Further, as shown in FIG.
The light intensity in the wavelength converter 500 is monitored so that the light output from 0 becomes a predetermined light output, and the pumping semiconductor laser 40 as the entire fiber optical amplifier (41, 42) is monitored.
It is preferable to further include a fiber output control device 407 for feedback-controlling the drive currents 1 and 43 respectively. In FIG. 8, the fiber output control device 407
Controls the semiconductor lasers 401 and 43 independently of each other, but may control only one of the semiconductor lasers 401 and 43 based on the light intensity detected by the wavelength converter 500. The fiber output control device 407 branches the laser light in the middle of the wavelength converter 500 and detects the intensity thereof.
A part of the laser light output from the emission end of the laser beam may be branched and its intensity may be detected. In FIG. 8, FIG.
The other components that are the same as those described above are given the same numbers, and descriptions thereof are omitted.

With such a configuration, the amplification factor of the fiber optical amplifier of each channel is made constant for each amplification stage, so that a biased load is not applied between the fiber optical amplifiers and the whole is uniform. Light intensity can be obtained. Further, by monitoring the light intensity in the wavelength conversion section 500, a predetermined predetermined light intensity is fed back to each amplification stage, and a desired ultraviolet light output can be stably obtained.

Although not shown in FIG. 8, at least one of the fiber output controllers 405, 406 and 407
One is connected to the single-wavelength oscillation laser (11 or 21) and the optical modulation element (12 or 22), respectively, and controls the temperature and current of the single-wavelength oscillation laser and drives the voltage pulse for driving to the optical modulation element. And it is possible to control the timing and magnitude of the voltage pulse.

Therefore, the at least one fiber output control device can control the intensity, the center wavelength, and the intensity of the pulsed light (the fundamental light or the visible light or the infrared light or the ultraviolet light whose wavelength has been converted at least once by the wavelength converter). And wavelength width,
Based on the detected value, the temperature of the single-wavelength oscillation laser is feedback-controlled to control the center wavelength and the wavelength width of the pulse light. Further, based on the detected value, the current control of the single wavelength oscillation laser and the control of the voltage pulse applied to the light modulation element are performed, and the intensity of the pulse light, the output interval, and the start and stop of the pulse output are performed. Control.

The at least one fiber output control device controls the switching between the pulse output and the continuous output of the single-wavelength oscillation laser, controls the output interval and the pulse width at the time of the pulse output, and controls the pulse light. At least one of the oscillation control of the single-wavelength oscillation laser and the control of the light modulation element is performed so as to compensate for the output fluctuation.

Although FIG. 8 is based on the premise that a large mode fiber optical amplifier is used, the pumping semiconductor laser (401) connected to the fiber optical amplifier described here is used.
) And the control of the single-wavelength oscillation laser and the light modulation element are performed by using the ultraviolet laser device according to the first and second embodiments described above without using a large-mode fiber optical amplifier (FIGS. 1 and 2). Can be applied as is.

The output ends of the final stage fiber optical amplifiers 19 and 25 in the first and second embodiments described above are bundled and formed into a required bundle shape (114, 2).
9). The number and shape of the bundles are determined according to the configuration of the wavelength conversion unit and the required shape of the light source. For example, this embodiment shows a case of a bundle having one circular cross section (114, 29, 501, 601 and the like). At this time, since the clad diameter of each fiber is about 125 μm, the diameter of the bundle at the output end where 128 fibers are bundled can be made about 2 mm or less. The bundle is the last stage E
Although it can be formed using the output terminal of DFA or YDFA as it is, the final stage EDFA or YDFA
It is also possible to couple an undoped fiber to A and form a bundle at its output end.

Further, as shown in FIG. 9, at the output end 423 of each fiber 422 at the last stage in the optical amplifier,
It is preferable that the diameter of the core 421 in the fiber 422 is gradually increased in a tapered shape toward the output end, and the power density (light intensity per unit area) at the output end face 423 is reduced. At this time, the shape of the taper is such that the expansion of the core diameter increases sufficiently gently toward the output end face 423, and when the amplified laser light propagates through the tapered portion, the propagation transverse mode in the fiber is preserved. The setting is made so that the transverse mode excitation can be sufficiently ignored (for example, about several mrad).

By setting in this manner, the power density of light at the output end face 423 of the fiber can be reduced, and damage to the fiber output end caused by laser light, which is the most problematic in fiber damage, is greatly suppressed. The effect is obtained. This effect is obtained when the power density of the laser light emitted from the output end of the fiber optical amplifier is higher (for example, as the light intensity is higher, the core diameter is smaller for the same power, or the number of channels for dividing the total power is smaller. A large effect can be obtained.

As shown in FIG. 10A, the laser beam is supplied to the output end 434 of the fiber 432 at the final stage together with the expansion of the core diameter or independently depending on the power density of the laser beam. Window member 43 of appropriate thickness to penetrate
It is preferable to dispose 3 closely. However, FIG.
In (a), the power density of the output light is reduced only by the window member 433 without increasing the diameter of the core 431 in the fiber.

Here, when there are a plurality of fiber outputs as in the first and second embodiments, in addition to the method shown in FIG. 10A in which a window member is provided for each fiber end, FIG.
As shown in (b), providing a common window member 443 at the output end 444 for each output group of each fiber optical amplifier 442 is also one embodiment of the present embodiment. However, although the diameter of the core 441 in the fiber is not enlarged in FIG. 10B, the enlargement of the core diameter may be used together.

The number of a plurality of fiber optical amplifiers in which one window member 443 is provided in common may be arbitrary. For example, the last stage fiber optical amplifier 1 shown in FIG. 1 or FIG.
The total number of 9 or 25, that is, 128 lines may be used. In addition,
The material of the window member (433 or 443) is appropriately selected (for example, an optical glass material such as BK7, a quartz material, or the like) in consideration of the transmittance in the wavelength region of the fundamental laser light, the adhesion to the fiber, and the like. For the close contact between the fiber and the window member, a method such as optical contact or fusion can be used.

With this configuration, the power density of the laser beam emitted from the window member becomes smaller than the power density in the fiber cores 431 and 441.
The effect of suppressing damage to the fiber output end by the laser beam can be obtained. By combining this with the expansion of the fiber core diameter at the output end, it is possible to solve the problem of damage to the fiber output end, which was a conventional problem.

In each of the above embodiments (FIGS. 1, 2, 4 and 8), the isolator 110, 111, 112, 26, 2
7, 404 etc. are inserted, and narrow band filters 113, 28, 403 are inserted in order to obtain good EDFA amplification characteristics. However, the location where the isolator or the narrow band filter is disposed or the number thereof is not limited to the above-described embodiment. For example, the required accuracy of various devices (such as an exposure device) to which the laser light source according to the present invention is applied is determined. It may be appropriately determined according to the situation, and at least one of the isolator and the narrow band filter may not be provided at all.

The narrow band filter only needs to have a high transmittance for only a desired single wavelength, and the transmission wavelength width of the filter is sufficient to be 1 pm or less. By using the narrow band filter in this manner, the ASE (Amplified Spontaneous Emitter) generated by the fiber amplifier is used.
is reduced, and a decrease in the amplification factor of the fundamental wave output due to the ASE from the fiber optical amplifier at the preceding stage can be suppressed.

In the above embodiment, the light modulating element 12
Or, monitor the intensity of the pulse light cut out in step 22 or the output of the fiber optical amplifier, and adjust the magnitude of the drive voltage pulse and the offset DC voltage applied to the optical modulation element so that the intensity becomes constant for each pulse. The intensity of the pulse light may be feedback controlled by adjusting the intensity. Further, the laser light generated from the large number of fiber optical amplifiers 19 or 25 is detected, and the delay time of the laser light in each channel and the oscillation interval of the laser light between the channels are monitored. By controlling the timing of the drive voltage pulse applied to the optical modulation element or controlling the TDM 23 in FIG. 2 so that each of the values becomes a predetermined value, the oscillation timing of the laser light at the output end of the fiber bundle is controlled. May be feedback controlled. Alternatively, the wavelength of the ultraviolet light generated from the wavelength converter 500 may be detected, and the temperature of the single-wavelength oscillation laser 11 or 21 may be adjusted based on the detected value to perform feedback control of the wavelength of the ultraviolet light.

Further, the intensity fluctuation of the pulse light cut out by the light modulation element 12 or 22 is detected, and a plurality of fiber optical amplifiers (13, 18, 19, or 24,
The so-called feed-forward control for controlling the gain in at least one stage of 25) may be performed. Further, among the above channels 0 to 127, the output (light intensity) of the channel having a short delay time, that is, the channel in which the pulse light is output earlier is detected, and the gain (or TDM23) of the fiber optical amplifier is determined based on the detected value. ), The output of the channel having a longer delay time than that channel, that is, the output of the channel in which the pulsed light is output with a delay, may be subjected to feedforward control. In particular, in the first embodiment shown in FIG. 1, the output may be controlled not in units of channels but in units of blocks having 32 channels. For example, at least one output of the first block may be controlled. The output of one channel may be detected, and the output of the channel in the second block may be controlled based on the detected value.

A third embodiment of the ultraviolet laser device according to the present invention will be described with reference to FIG. The ultraviolet light generation device according to the present embodiment includes a laser light generation unit that includes a single wavelength oscillation laser 31 and generates a single wavelength laser light, an optical amplifier that includes fiber optical amplifiers 33 and 34 and amplifies incident light, and An ultraviolet laser device that includes a wavelength converter (not shown) that converts the wavelength of the amplified light, and generates a laser beam having the same output wavelength (193 nm) as the ArF excimer laser or the same output wavelength (157 nm) as the F ₂ laser. Is provided.

In this embodiment, the ultraviolet laser device shown in FIG. 3 includes a single-wavelength oscillation laser 31 for generating a single-wavelength laser beam, and the optical output of the single-wavelength oscillation laser 31 is a fiber optical amplifier. Amplified by 33,34. The output of the fiber optical amplifier 34 is, for example, as shown in FIG.
The amplified laser light is incident on the wavelength converters (602 to 611) shown in FIG. The emission ends of the fiber optical amplifier 34 in FIG. 3 correspond to the fiber bundle emission ends 501 and 601 shown in FIGS. The wavelength conversion unit includes a set of nonlinear optical crystals 602,
604, 609, 611, etc., and convert the fundamental wave emitted from the optical amplifiers (31-36) to ultraviolet light. The wavelength conversion unit according to the present invention will be described in detail as Embodiments 4 to 7 later in the embodiment.

Hereinafter, the present embodiment will be described in more detail. As the single-wavelength oscillation laser 31 oscillating at a single wavelength shown in FIG.
An InGaAsP, DFB semiconductor laser having a W output of 30 mW is used. Since this laser basically oscillates in a single longitudinal mode, its oscillation spectral line width can be suppressed to 0.01 pm or less.

Light output (continuous light) of this semiconductor laser 31
Is converted into pulse light by a light modulation element 32 such as an electro-optic light modulation element or an acousto-optic light modulation element. In the present configuration example, as an example, a case where the light modulation element 32 modulates the pulse light into a pulse light having a pulse width of 1 ns and a repetition frequency of 100 kHz will be described. As a result of performing such light modulation, the peak output of the pulse light output from the light modulation element 32 is 30 mW, and the average output is 3 μW.

The output light pulsed in the same manner as in the first and second embodiments is amplified by a fiber optical amplifier having one or more stages of EDFA (erbium-doped fiber optical amplifier). In the present embodiment, as an example, the case where the amplification is performed in a total of 58 dB (667000 times) by the two-stage fiber optical amplifiers 33 and 34 has been described. In this case, the fiber optical amplifier 3
The average output at the output terminal of No. 4 is 2W. This output end can be formed using the output end of the final stage fiber optical amplifier 34 as it is, but it is also possible to couple an undoped fiber to the final stage fiber optical amplifier 34. Further, in the present embodiment, a configuration example is shown in which isolators 35 and 36 are appropriately inserted into each connection part in order to avoid the influence of return light.

The wavelength 1.544, which is the output of this optical amplifier,
The μm single-wavelength pulsed laser light is converted into an ultraviolet light pulse output having a narrow spectral line width by a wavelength converter (described later in detail) using a nonlinear optical crystal. In the optical amplifiers (31 to 36) according to the present embodiment, the output ends of the optical amplifiers are constituted by a single fiber optical amplifier 34.
A plurality of fiber optical amplifiers (33, 34) are prepared together with the plate waveguide type splitter (16) used in (FIG. 1) or the TDM (23) used in Embodiment 2, and the fiber optical amplifiers 34 are bundled. A fiber bundle may be formed. At this time, by adjusting the timing of the drive voltage pulse applied to the optical modulation element 32 provided in each of the plurality of optical amplifiers, the oscillation interval of the pulse light emitted from the plurality of optical amplifiers can be adjusted.
For example, as pulse light is emitted sequentially at equal time intervals,
It is preferable to shift the light emission timing for each optical amplifier.

Further, also in this embodiment, it is possible to apply the modifications of the first and second embodiments. For example, the single-wavelength oscillation laser 31 may be pulse-oscillated, or only the current control of the single-wavelength oscillation laser 31 may be performed.
Alternatively, the output interval (pulse cycle) of the pulse light may be changed by using both the current control and the control of the light modulation element 32.

Next, an embodiment of the wavelength converter used in each of the first to third embodiments will be described. FIG.
1A to 1D show a configuration example of a wavelength conversion unit according to the present invention as a fourth embodiment. These all correspond to the output end 501 of the fiber bundle (114 in the first embodiment, 29 in the second embodiment, and the like, but may be the output end of the single fiber (34) in the third embodiment. ), The fundamental wave having a wavelength of 1.544 nm is converted into an eighth harmonic (harmonic wave) using a nonlinear optical crystal to generate 193 nm ultraviolet light having the same wavelength as the ArF excimer laser. This is an example.

In FIG. 11A, the fundamental wave having a wavelength of 1.544 nm (frequency ω) output from the fiber bundle output end 501 is nonlinear optical crystals 502, 503, and 50.
4 is transmitted from left to right in the figure and output. When the fundamental wave passes through the nonlinear optical crystal 502, the second harmonic generation generates twice the frequency ω of the fundamental wave, that is, the frequency 2ω.
A second harmonic (the wavelength is の of 772 nm) is generated. The generated second harmonic travels rightward, and the next nonlinear optical crystal 50
3 is incident. Here, the second harmonic is generated again, and a fourth harmonic having a frequency 4ω (wavelength is 1/4 of 386 nm) which is twice the frequency 2ω of the incident wave, that is, four times the fundamental wave is generated. The generated fourth harmonic further proceeds to the right nonlinear optical crystal 504 where the second harmonic is generated again.
An eighth harmonic having a frequency 8ω which is twice the frequency 4ω of the incident wave, that is, eight times the fundamental wave (the wavelength is ８
m).

As the nonlinear optical crystal used for the wavelength conversion, for example, a LiB ₃ O ₅ (LBO) crystal is used for the conversion crystal 502 from the fundamental wave to the second harmonic, and a conversion crystal for converting the second harmonic to the fourth harmonic. 503 is a LiB ₃ O ₅ (LBO) crystal,
Sr ₂ Be ₂ B ₂ O ₇ (SBBO) crystal is used for the conversion crystal 504 into the harmonic. Here, the conversion from the fundamental wave to the second harmonic wave using the LBO crystal is performed by phase matching for wavelength conversion.
Method by temperature control of BO crystal, Non-Critical Phase M
atching: Uses NCPM. NCPM is a method of calculating the angular shift (Walk-of) between the fundamental wave and the second harmonic in the nonlinear optical crystal.
Since f) does not occur, it is possible to convert to a second harmonic wave with high efficiency, and the generated second harmonic wave is advantageous because it does not undergo beam deformation due to walk-off.

FIG. 11B shows a fundamental wave (wavelength 1.544).
μm) → 2nd harmonic (wavelength 772 nm) → 3rd harmonic (wavelength 51
5nm) → 6th harmonic (wavelength 257nm) → 8th harmonic (wavelength 1)
(93 nm).

In the first-stage wavelength converter 507, an LBO crystal is used in the above-mentioned NCPM for conversion of generation of a second harmonic from a fundamental wave to a second harmonic. Wavelength conversion unit (LBO crystal)
A reference numeral 507 transmits a part of the fundamental wave without converting the wavelength, converts the wavelength of the fundamental wave to generate a second harmonic, and converts the fundamental wave and the second harmonic into a wave plate (for example, a half wave plate) At 508, a delay of one half wavelength and one wavelength is given, and only the polarization of the fundamental wave is rotated by 90 degrees. The fundamental wave and the second harmonic wave respectively enter the second-stage wavelength converter 510 through the lens 509.

The second-stage wavelength converter 510 generates a third harmonic (wavelength 515) from the second harmonic generated by the first-stage wavelength converter 507 and the fundamental wave transmitted without conversion by sum frequency generation.
nm). Although an LBO crystal is used as the wavelength conversion crystal, it is used in an NCPM having a different temperature from the wavelength conversion unit (LBO crystal) 507 in the first stage. Wavelength converter 51
The third harmonic obtained at 0 and the second harmonic transmitted without wavelength conversion are separated by a dichroic mirror 511,
The third harmonic reflected by the dichroic mirror 511 is
The light enters the third-stage wavelength converter 514 through the lens 513. The wavelength converter 514 is a β-BaB ₂ O ₄ (BBO) crystal, where the third harmonic is the sixth harmonic due to the generation of the second harmonic.
(Wavelength 257 nm).

The sixth harmonic obtained by the wavelength conversion unit 514 and the second harmonic transmitted through the dichroic mirror 511 and passed through the lens 512 are coaxially synthesized by the dichroic mirror 516 and the fourth wavelength The light enters the conversion unit 517.
BBO crystal is used for the wavelength conversion unit 517,
Eighth harmonic (wavelength 193 nm) by sum frequency generation from harmonics
Get. In the configuration of FIG. 11B, a CsLiB ₆ O ₁₀ (CLBO) crystal can be used instead of the BBO crystal as the wavelength conversion crystal of the fourth-stage wavelength conversion section 517.

In the present embodiment, the second-stage wavelength converter 5
The third harmonic and the second harmonic obtained in 10 are branched by the dichroic mirror 511, and the sixth harmonic obtained in the third-stage wavelength converter 514 and the second harmonic are obtained in the second-stage wavelength converter 510. The second harmonic is combined with the dichroic mirror 516,
It was configured to be incident on the fourth-stage wavelength converter 517. Here, assuming that the characteristics of the dichroic mirror 511 are inverted, that is, the third harmonic wave is transmitted and the second harmonic wave is reflected, the third-stage wavelength converter 514 is the same as the second-stage wavelength converter 510. It may be arranged on the optical axis. At this time, the characteristics of the dichroic mirror 516 also need to be inverted. As described above, one of the sixth harmonic and the second harmonic passes through the branch optical path and the wavelength conversion unit 517 in the fourth stage.
In the configuration in which the second and third harmonics are incident on the wavelength conversion unit 517 at the fourth stage, respectively.
12 can be arranged in different optical paths.

Since the sixth harmonic generated in the third-stage wavelength converter 514 has an elliptical cross-sectional shape due to the walk-off phenomenon, the fourth-stage wavelength converter 517 obtains good conversion efficiency. For this purpose, it is desirable to perform beam shaping of the sixth harmonic. Therefore, as in the present embodiment, the condensing lens 51
By disposing the lenses 5 and 512 in separate optical paths, for example, a pair of cylindrical lenses can be used as the lens 515, and the beam shaping of the sixth harmonic can be easily performed. For this reason, it is possible to improve the overlap with the second harmonic wave in the fourth-stage wavelength conversion unit (BBO crystal) 517 and improve the conversion efficiency.

The configuration between the second-stage wavelength converter 510 and the fourth-stage wavelength converter 517 is not limited to that shown in FIG. Any configuration may be used as long as the optical path lengths of the sixth harmonic and the second harmonic are equal so that the second harmonic and the second harmonic enter simultaneously. Further, for example, the second-stage wavelength converter 510
The third and fourth wavelength conversion units 514 on the same optical axis as
The third-stage wavelength converter 514 converts only the third harmonic into a sixth harmonic by generating the second harmonic, and enters the fourth-stage wavelength converter 517 together with the second harmonic that is not wavelength-converted. The dichroic mirror 5
It is not necessary to use 11, 516.

FIG. 11C shows a fundamental wave (wavelength 1.544).
μm) → 2nd harmonic (wavelength 772 nm) → 4th harmonic (wavelength 38)
6 nm) → 6th harmonic (wavelength 257 nm) → 8th harmonic (wavelength 1
(93 nm).

In the first-stage wavelength conversion section 518, an LBO crystal is used as the wavelength conversion crystal, and the LBO crystal is used in the NCPM to convert the wavelength of the fundamental wave to the second harmonic. The second harmonic generated from the first-stage wavelength converter 518 passes through the condenser lens 519 and passes through the second-stage wavelength converter 52.
Incident at 0.

In the second-stage wavelength conversion section 520, an LBO crystal is used as the wavelength conversion crystal, and the second harmonic generated by the first-stage wavelength conversion section 518 is converted into a fourth harmonic (wavelength). 386 nm). The fourth harmonic obtained by the wavelength converter 520 and the wavelength converter 5
The second harmonic transmitted through 20 is a dichroic mirror 5
The fourth harmonic reflected there is passed through the condenser lens 524 and reaches the dichroic mirror 525. On the other hand, the light transmitted through the dichroic mirror 521
The harmonic wave is rotated by 90 ° in the polarization direction by the half-wave plate 522, passes through the condenser lens 523, reaches the dichroic mirror 525, and is coaxially synthesized with the second harmonic wave passing through the branch optical path. The light enters the third-stage wavelength converter 526.

In the third-stage wavelength conversion section 526, a BBO crystal is used as the wavelength conversion crystal, and the fourth harmonic generated in the second-stage wavelength conversion section 520 and the wavelength conversion section 520 without wavelength conversion are used. A 6th harmonic (wavelength: 257 nm) is obtained from the 2nd harmonic that has passed through by generating a sum frequency. Wavelength converter 52
0 is separated from the second harmonic transmitted through the wavelength converter 520 without wavelength conversion by the dichroic mirror 527, and the second harmonic reflected here is converted into a half-wave plate 528. Then, the polarization direction is rotated by 90 °, and reaches the dichroic mirror 531 through the condenser lens 529. On the other hand, dichroic mirror 527
Passes through the condenser lens 530 and reaches the dichroic mirror 531, where it is coaxially combined with the second harmonic passing through the branch optical path and becomes the fourth-stage wavelength converter 532.
Incident on.

In the fourth-stage wavelength conversion section 532, a BBO crystal is used as the wavelength conversion crystal, and the sixth harmonic generated in the third-stage wavelength conversion section 526 and the wavelength conversion section 526 are not converted. And an 8th harmonic (wavelength: 193 nm) is obtained from the 2nd harmonic transmitted through. In the above configuration, it is possible to use a CLBO crystal instead of a BBO crystal as the wavelength conversion crystal of the fourth-stage wavelength conversion section 532.

In this embodiment, dichroic mirrors (521 or 527) are arranged after the second-stage and third-stage wavelength converters 520 and 526, respectively, and the wavelength converters (520 or 526) are arranged. So that a pair of harmonics (2nd and 4th harmonics or 2nd and 6th harmonics) emitted from the optical path enter the next-stage wavelength converter (526 or 532) through different optical paths. 11B, the third-stage wavelength converter 526 may be arranged on the same optical axis as the other wavelength converters 518, 520, and 532, as in the description of FIG.・ Mirrors 521, 5
It is not necessary to use 25, 527, 531 or the like.

In this embodiment, the fourth and sixth harmonics generated by the second and third wavelength converters 520 and 526 have oval cross sections due to the walk-off phenomenon. . Therefore, in order to obtain good conversion efficiency in the third and fourth stage wavelength converters 526 and 532 which receive this beam as an input, the fourth harmonic wave and the sixth harmonic wave which are incident beams are required.
It is desirable to shape the beam shape of the harmonic wave to make the overlap with the harmonic wave beam good. By placing the condenser lenses 523 and 524 and 529 and 530 in separate optical paths as in this embodiment, for example, the lenses 524 and
A cylindrical lens pair can be used as 30, and beam shaping of the fourth harmonic and the sixth harmonic can be easily performed. For this reason, the third and fourth stage wavelength converters 526 and 532 have good overlap with the second harmonic, respectively, and can increase the conversion efficiency.

The second and fourth harmonics generated from the second-stage wavelength converter 520 are simultaneously output from the third-stage wavelength converter 52.
It is only necessary that the optical path lengths of the second harmonic and the fourth harmonic are the same so as to be incident on the two wavelength converters 520, 5, and 5.
The configuration between 26 is not limited to FIG.
This is the same between the third-stage wavelength converter 526 and the fourth-stage wavelength converter 532.

FIG. 11D shows a fundamental wave (wavelength 1.544).
μm) → 2nd harmonic (wavelength 772 nm) → 3rd harmonic (wavelength 51
5nm) → 4th harmonic (wavelength 386nm) → 7th harmonic (wavelength 2)
21 shows a case where wavelength conversion is performed in the order of 21 nm) to 8th harmonic (wavelength 193 nm).

In the first-stage wavelength conversion section 533, an LBO crystal is used as the wavelength conversion crystal, and the LBO crystal is used in the NCPM to convert the wavelength of the fundamental wave to the second harmonic. The fundamental wave transmitted without wavelength conversion by the wavelength conversion unit 533 and the second harmonic generated by the wavelength conversion are separated by a wavelength plate 534.
Respectively, a delay of one half wavelength and one wavelength is given, and only the fundamental wave rotates its polarization direction by 90 degrees. The second-stage wavelength conversion unit 536 uses an LBO crystal as the wavelength conversion crystal, and the LBO crystal is used in the NCPM having a different temperature from the first-stage wavelength conversion unit (LBO crystal) 533. The wavelength converter 536 generates a third harmonic (wavelength 515 nm) from the second harmonic generated in the first-stage wavelength converter 533 and the fundamental wave transmitted through the wavelength converter 533 without wavelength conversion. Get)

The third harmonic obtained by the wavelength converter 536 and the fundamental wave and the second harmonic transmitted through the wavelength converter 536 without wavelength conversion are separated by the dichroic mirror 537 and reflected there. The third harmonic is collected by a condenser lens 54.
0 and passes through the dichroic mirror 543 to enter the fourth-stage wavelength converter 545. On the other hand, the fundamental wave and the second harmonic transmitted through the dichroic mirror 537 enter the third-stage wavelength converter 539 through the condenser lens 538.

In the third-stage wavelength converter 539, an LBO crystal is used as the wavelength conversion crystal, and the fundamental wave is transmitted through the LBO crystal without wavelength conversion, and the second harmonic is converted to the second harmonic by the LBO crystal. Fourth harmonic (wavelength 386)
nm). The fourth harmonic obtained by the wavelength conversion unit 539 and the fundamental wave transmitted therethrough are separated by a dichroic mirror 541, and the fundamental wave transmitted therethrough passes through a condenser lens 544, and the dichroic mirror 54
The light is reflected by 6 and enters the fifth-stage wavelength converter 548.
On the other hand, the fourth harmonic reflected by the dichroic mirror 541 reaches the dichroic mirror 543 through the condenser lens 542, where the dichroic mirror 537
The light is combined coaxially with the third harmonic wave reflected by the light source and enters the fourth-stage wavelength converter 545.

The fourth-stage wavelength converter 545 uses a BBO crystal as its wavelength conversion crystal, and obtains a seventh harmonic (wavelength 221 nm) from the third harmonic and the fourth harmonic by generating a sum frequency. The seventh harmonic obtained by the wavelength conversion unit 545 is
47 and dichroic mirror 546
Then, the light is synthesized coaxially with the fundamental wave transmitted through the dichroic mirror 541 and enters the fifth-stage wavelength conversion unit 548.

The fifth-stage wavelength converter 548 uses an LBO crystal as its wavelength conversion crystal, and obtains an eighth harmonic (wavelength 193 nm) from the fundamental wave and the seventh harmonic by generating a sum frequency. In the above configuration, the seventh harmonic generation BBO crystal 54
Instead of the LBO crystal 548 for generating fifth and eighth harmonics, C
It is also possible to use LBO crystals.

In this embodiment, the fourth-stage wavelength converter 545 is used.
Since the third harmonic and the fourth harmonic enter through different optical paths, the lens 540 for condensing the third harmonic and the lens 542 for condensing the fourth harmonic can be placed on separate optical paths. . The cross-sectional shape of the fourth harmonic generated by the third-stage wavelength converter 539 is an elliptical shape due to the walk-off phenomenon. Therefore, in order to obtain good conversion efficiency in the fourth-stage wavelength converter 545, it is desirable to perform beam shaping of the fourth harmonic. In this embodiment, since the condenser lenses 540 and 542 are arranged in separate optical paths, for example, a pair of cylindrical lenses can be used as the lens 542, and the beam shaping of the fourth harmonic can be easily performed. . For this reason, it is possible to improve the overlap with the third harmonic wave in the fourth-stage wavelength conversion unit (BBO crystal) 545 and improve the conversion efficiency.

Further, in this embodiment, a lens 544 for condensing the fundamental wave incident on the fifth-stage wavelength converter 548,
The lens 547 that collects the harmonic can be placed in a separate optical path. The seventh harmonic generated by the fourth-stage wavelength converter 545 has an elliptical cross-sectional shape due to the Walk-off phenomenon. Therefore, in order to obtain good conversion efficiency in the fifth-stage wavelength converter 548, it is preferable to perform beam shaping of the seventh harmonic. In the present embodiment, the condenser lenses 544 and 54
Since the lenses 7 can be arranged in different optical paths, for example, a pair of cylindrical lenses can be used as the lens 547, and the beam shaping of the seventh harmonic can be easily performed. Therefore, the fifth-stage wavelength conversion unit (LBO crystal) 5
It is possible to make the overlap with the fundamental wave at 48 good and increase the conversion efficiency.

The configuration between the second-stage wavelength converter 536 and the fourth-stage wavelength converter 545 is not limited to that shown in FIG. 11D, but is generated by the wavelength converter 536 to generate dichroic signals. The third harmonic reflected by the mirror 537 and the dichroic mirror 53 generated by the wavelength converter 536
The two optical path lengths between the two wavelength converters 536 and 545 are equal so that the second harmonic transmitted through 7 and the fourth harmonic obtained by wavelength conversion by the wavelength converter 539 simultaneously enter the wavelength converter 545. Any configuration may be used as long as the configuration is satisfied. This is the same between the third-stage wavelength converter 539 and the fifth-stage wavelength converter 548.

FIGS. 12A to 12D show FIGS.
The wavelength conversion efficiency at each stage for each channel and the average output of the eighth harmonic (wavelength 193 nm) obtained for each channel are shown for the wavelength conversion unit shown in FIG. As described in the above embodiment, the output of the fundamental wave is the output terminal of each channel, and has a peak power of 20 kW, a pulse width of 1 ns, a pulse repetition frequency of 100 kHz, and an average output of 2 W. As a result, the average output of the eighth harmonic (wavelength 193 nm) per channel is 229 mW in the wavelength converter of FIG. 11A, 38.3 mW in the wavelength converter of FIG. 11B, and FIG. 11C. 40.3
mW, and 45.9 mW in the wavelength converter of FIG. Therefore, the average output from the bundle including all 128 channels is 29 W in FIG.
FIG. 11B shows 4.9 W, FIG. 11C shows 5.2 W, and FIG.
In the case of 1 (d), the power is 5.9 W, and the wavelength 193 of any output from the wavelength converter is sufficient for the light source for the exposure apparatus.
nm ultraviolet light can be provided.

Of these embodiments, the configuration shown in FIG. 11A is the simplest and has the highest conversion efficiency. Therefore, the number of channels of the fiber optical amplifier is reduced as compared with the first and second embodiments (128 channels).
Even if a bundle is configured with the number of channels of ２〜 to １ ／ or a fundamental wave output lower than the fundamental wave output shown in the present embodiment, an output sufficient for a light source for an exposure apparatus can be obtained. It is possible to provide ultraviolet light having a wavelength of 193 nm.

In the configuration shown in FIG. 11D, the number of stages of the wavelength conversion unit is five, which is the largest among these embodiments.
The conversion efficiency to the same is similar to that of the embodiment of FIGS. 11B and 11C, and almost the same ultraviolet light output can be obtained. In the configurations of FIGS. 11B and 11C, the BBO crystal is used to generate the eighth harmonic (193 nm).
There is an absorption of the eighth harmonic (193 nm) by the BBO crystal,
Damage to the BBO crystal can be a problem. On the other hand, in the configuration of FIG. 11D, an LBO crystal can be used to generate an eighth harmonic (193 nm). At present, this LBO crystal is readily available as a commercial product, and has a very small absorption coefficient of ultraviolet light of 193 nm, and does not cause a problem of optical damage to the crystal. is there.

In the generation section of the eighth harmonic (for example, the wavelength of 193 nm), the LBO crystal is used after being angularly phase-matched.
Due to the large phase matching angle, the effective nonlinear optical constant (d
eff) becomes smaller. Therefore, it is preferable to provide a temperature control mechanism for the LBO crystal and use the LBO crystal at a high temperature. Thereby, the phase matching angle can be reduced, that is, the above constant (deff) can be increased,
Eighth harmonic generation efficiency can be improved.

Although the preferred embodiment of the wavelength converter for generating the eighth harmonic from the fundamental wave has been described above, the wavelength converter of the present invention is restricted only to this embodiment. Instead, the same effect can be obtained if the configuration generates an eighth harmonic of 1.544 μm, which is the fundamental wave. For example, fundamental wave (wavelength 1.544 μm) → second harmonic (wavelength 772 nm) → third harmonic (wavelength 515 nm) → fourth harmonic (wavelength 386 nm) → sixth harmonic (wavelength 257 nm) → seventh harmonic (wavelength 221 nm) → 8
The same effect can be obtained by performing wavelength conversion in the order of harmonics (wavelength 193 nm).

At this time, as the nonlinear optical crystal used for the wavelength conversion, for example, an LBO crystal is used for converting a fundamental wave to a second harmonic, and an LBO crystal is used for converting a second harmonic to a fourth harmonic. The BBO crystal is used for generating the sixth harmonic by summing the second and fourth harmonics, the BBO crystal is used for generating the seventh harmonic by generating the sum of the fundamental wave and the sixth harmonic, and the fundamental wave is used. 7
Generation of the eighth harmonic by sum frequency generation with the harmonic can be achieved by using an LBO crystal. Also in this case, since the LBO crystal can be used for the generation of the eighth harmonic, there is an advantage in that damage to the crystal is not a problem.

By configuring the wavelength converter as described in the fourth embodiment, the fundamental wave having a wavelength of 1.544 μm generated by the fundamental wave generator can be converted into ultraviolet light having a wavelength of 193 nm. .

Next, FIG. 13 shows another embodiment of the wavelength converter according to the present invention as a fifth embodiment. This corresponds to the output end 601 of the fiber bundle (11 in the first embodiment).
4, a fundamental wave having a wavelength of 1.57 μm, which is emitted from (e.g., 29 in Embodiment 2), is subjected to harmonic generation of a 10th harmonic using a nonlinear optical crystal, and is 157 nm, which is the same wavelength as the F ₂ laser. 2 shows an example of a configuration for generating ultraviolet light. Note that the fundamental wave output unit in the present embodiment includes:
Any of the first to third embodiments described so far, or a combination thereof can be used.

In the configuration example of the wavelength conversion section shown in FIG. 13, the fundamental wave (wavelength: 1.57 μm) → the second harmonic wave (wavelength: 785 nm)
→ 4th harmonic (wavelength 392.5nm) → 8th harmonic (wavelength 19)
This shows a case where wavelength conversion is performed in the order of 6.25 nm) to 10th harmonic (wavelength: 157 nm). In this embodiment, in each wavelength conversion stage from the generation of the second harmonic to the generation of the eighth harmonic, the second harmonic generation of the wavelength incident on each wavelength conversion stage is performed.

In this example, as a nonlinear optical crystal used for wavelength conversion, an LBO crystal is used to generate a second harmonic by generating a second harmonic from a fundamental wave in the wavelength converter 602, and the wavelength converter 604 The LBO crystal is used for the generation of the fourth harmonic by the generation of the second harmonic from the second harmonic. Further, an Sr ₂ Be ₂ B ₂ O ₇ (SBBO) crystal is used for generation of an eighth harmonic by generation of a second harmonic from a fourth harmonic in the wavelength converter 609, and the second harmonic and the eighth harmonic in the wavelength converter 611 are used. An SBBO crystal is used to generate a tenth harmonic (wavelength: 157 nm) by sum frequency generation from the harmonic.

The second harmonic generated from the wavelength converter 602 enters the wavelength converter 604 through the condenser lens 603, and the wavelength converter 604 converts the second harmonic into a second harmonic that is not wavelength-converted. And generate. Next, the dichroic
The second harmonic transmitted through the mirror 605 passes through the condenser lens 606, is reflected by the dichroic mirror 607, and enters the wavelength converter 611. On the other hand, the fourth harmonic reflected by the dichroic mirror 605 is
8 and enters the wavelength converter 609, and the eighth harmonic generated here passes through the condenser lens 610 and the dichroic mirror 607 and enters the wavelength converter 611. Further, the wavelength conversion unit 611 includes a dichroic mirror 607.
A 10th harmonic (wavelength: 157 nm) is generated from the 2nd harmonic and the 8th harmonic that are coaxially synthesized by the above.

In the present embodiment, the second and fourth harmonics generated by the second-stage wavelength converter 604 are branched by the dichroic mirror 605 to transmit the second and fourth harmonics.
Although the fourth harmonic wave and the eighth harmonic wave obtained by wavelength-converting the fourth harmonic wave by the wavelength conversion unit 609 enter the fourth wavelength conversion unit 611 through different optical paths, the dichroic mirror is used. Four wavelength converters 602, 604, 609, and 611 may be arranged on the same optical axis without using 605 and 607.

However, in the present embodiment, the second-stage wavelength converter 6
The fourth harmonic generated in 04 has an oval cross section due to the Walk-off phenomenon. Therefore, in order to obtain good conversion efficiency in the fourth-stage wavelength conversion section 611 that receives this beam as an input, the beam shape of the fourth harmonic wave that becomes the incident beam is shaped to improve the overlap with the second harmonic wave. Is desirable.
In the present embodiment, since the condenser lenses 606 and 608 can be arranged in separate optical paths, for example, a cylindrical lens can be used as the lens 608.
The beam shaping of the harmonic wave can be easily performed. For this reason, it is possible to improve the overlap with the second harmonic in the fourth-stage wavelength converter 611, and to increase the conversion efficiency.

By configuring the wavelength converter as described in the fifth embodiment, it is possible to convert the wavelength of the fundamental wave of 1.57 μm generated by the fundamental wave generator into the ultraviolet light of the wavelength of 157 nm. it can.

FIG. 14 shows another embodiment of the wavelength conversion section according to the present invention as a sixth embodiment. This constitutes a fundamental wave generator, for example, as shown in the second embodiment, and is emitted from the output end 701 of the fiber bundle (corresponding to 114 in the first embodiment, 29 in the second embodiment, and the like). This is an example of a configuration in which a fundamental wave having a wavelength of 1.099 μm is subjected to seventh harmonic generation using a nonlinear optical crystal to generate 157 nm ultraviolet light having the same wavelength as the F ₂ laser. Note that the fundamental wave output unit in the present embodiment can use any one of the first to third embodiments described above or a combination thereof.

In the configuration example of the wavelength converter shown in FIG. 14, the fundamental wave (wavelength 1.099 μm) → the second harmonic wave (wavelength 549.5)
In this case, the wavelength conversion is performed in the order of (nm) → third harmonic (wavelength 366.3 nm) → fourth harmonic (wavelength 274.8 nm) → seventh harmonic (wavelength 157 nm). In this embodiment, the second harmonic generation or the sum frequency generation of the incident light is performed in each wavelength converter.

In this example, as a nonlinear optical crystal used for wavelength conversion, an LBO crystal is used to generate a second harmonic by generating a second harmonic from a fundamental wave in the wavelength converter 702. The LBO crystal is used to generate the third harmonic by sum frequency generation from the fundamental wave and the second harmonic in the above. Further, a BBO crystal is used to generate the fourth harmonic by generating the second harmonic from the second harmonic in the wavelength converter 710, and the third harmonic and the fourth harmonic are used by the wavelength converter 712 to generate the seventh harmonic by the sum frequency generation. An SBBO crystal is used to generate waves.

The fundamental wave and the second harmonic wave generated from the wavelength conversion section (LBO crystal) 702 are incident on the half-wave plate 703, and only the fundamental wave has its polarization direction rotated by 90 degrees and is condensed. The light enters the wavelength conversion unit (LBO crystal) 705 through the lens 704. The wavelength conversion unit 705 obtains a third harmonic by generating a sum frequency from the fundamental wave and the second harmonic,
The second harmonic is transmitted without wavelength conversion. The second harmonic and the third harmonic generated from the wavelength converter 705 are branched by a dichroic mirror 706, and the third harmonic transmitted therethrough passes through a condenser lens 707 and passes through a dichroic mirror 70.
The light is reflected at 8 and enters the wavelength converter 712. On the other hand, the second harmonic reflected by the dichroic mirror 706 passes through the condenser lens 709 and enters the wavelength converter 710. The wavelength converter 710 converts the second harmonic into a fourth harmonic by generating a second harmonic. appear. This fourth harmonic is collected by a condenser lens 711,
Then, the light enters the wavelength converter 712 through the dichroic mirror 708. The wavelength converter 712 generates a seventh harmonic from the third harmonic and the fourth harmonic by sum frequency generation.

In the present embodiment, the second harmonic and the third harmonic generated from the second-stage wavelength converter 705 are branched by the dichroic mirror 706 to transmit the third and third harmonics.
Although the harmonic and the fourth harmonic obtained by wavelength-converting the second harmonic by the wavelength converter 710 are configured to enter the fourth-stage wavelength converter 712 through different optical paths, the dichroic mirror is used. Four wavelength converters 702, 705, 710, 712 may be arranged on the same optical axis without using 706, 708.

However, in this embodiment, the third-stage wavelength converter 7
The cross-sectional shape of the fourth harmonic generated at 10 is oblong due to the walk-off phenomenon. Therefore, in order to obtain good conversion efficiency in the fourth-stage wavelength conversion unit 712 that receives this beam as an input, the beam shape of the fourth harmonic wave that becomes the incident beam is shaped to improve the overlap with the third harmonic wave. Is desirable.
In the present embodiment, since the condenser lenses 707 and 711 can be arranged in separate optical paths, for example, a cylindrical lens can be used as the lens 711.
The beam shaping of the harmonic wave can be easily performed. For this reason, it is possible to improve the overlap with the third harmonic in the fourth-stage wavelength converter 712 and to increase the conversion efficiency.

By configuring the wavelength converter as described in the sixth embodiment, it is possible to convert the wavelength of a fundamental wave of 1.099 μm generated by the fundamental wave generator to ultraviolet light of a wavelength of 157 nm. it can.

Next, another configuration example of an optical amplifier and a wavelength conversion section according to the present invention is shown in FIG. 15 as a seventh embodiment. In FIG. 15, the wavelength conversion unit has a plurality of parallel optical path configurations (square arrangement of four optical paths in the example of the figure), and in accordance with this, the output terminals of a large number of fiber optical amplifiers 19 or 25 are formed into four bundles (output groups). While dividing the light, the condensing optical elements corresponding to the four fiber bundle output ends,
And an embodiment in which a wavelength converter is provided. In this example, FIG.
Alternatively, since it is assumed that the optical amplifier shown in FIG. 2 is used, 32 fiber optical amplifiers 19 or 25 are bundled in one fiber bundle. Note that the bundle is the final stage EDFA output terminal or YDF
A output end can be formed as it is, but an undoped fiber is coupled to the final stage EDFA, etc.
It is also possible to form a bundle at its output end.

Also, the fiber optical amplifier 19 or 25
In the case where a plurality of fiber bundles are formed by dividing the output end of the optical fiber into a plurality of fiber bundles, the output The (fiber optical amplifier) is preferably configured to be bundled into different fiber bundles. For example, in the order in which laser light is emitted,
No. 0 for 8 fiber optical amplifiers (19 or 25)
No. 0 to 4, No. 127
, 124 are bundled as a first fiber bundle, and Nos. 1, 5, 9,.
, 125 fiber optical amplifiers are bundled as a second fiber bundle, and Nos. 3, 6, 10,.
6 are bundled as a third fiber bundle, and the fiber optical amplifiers Nos. 4, 7, 11,..., 127 are bundled as a fourth fiber bundle. This makes it possible to equally divide the time interval of the pulse light incident on the wavelength converter (non-linear optical crystal) arranged corresponding to each fiber bundle.

Now, as shown in FIG. 15, the fundamental wave emitted from the output end 841 of the optical amplifier (FIG. 1 or FIG. 2) composed of four fiber bundles has three stages of wavelength converters 842 in this example. Wavelength conversion is performed at 843 and 844, respectively. In this example, any of the wavelength converters (FIGS. 11, 13, and 14) described in the fourth to sixth embodiments can be used, but here, the wavelength converter shown in FIG. That is, an example in which the fundamental wave (wavelength: 1.544 μm) is converted into ultraviolet light having a wavelength of 193 nm by a three-stage nonlinear optical crystal (502 to 504) will be described. Accordingly, the fundamental wave having a wavelength of 1.544 μm (frequency ω) passes through the nonlinear optical crystals 842, 843, and 844 from left to right in the drawing, so that the second harmonic, the fourth harmonic,
The wavelength is sequentially converted to the eighth harmonic (wavelength 193 nm) and output.

In FIG. 15, the fundamental wave (wavelength: 1.544 μm) emitted from the output end 841 of the optical amplifier composed of four fiber bundles passes through the condenser lenses 845 provided corresponding to the four fiber bundles. Then, the light enters a wavelength converter (nonlinear optical crystal) 842, where a second harmonic is generated, which is twice the frequency ω of the fundamental wave, that is, a second harmonic having a frequency 2ω (wavelength 772 nm). The second harmonic generated by the wavelength converter 842 travels rightward and passes through the condenser lens 846 to enter the next wavelength converter (nonlinear optical crystal) 843. Here, the second harmonic generation is performed again, and the frequency 4ω (wavelength 386n) is twice the frequency 2ω of the incident wave (the second harmonic), that is, four times the fundamental wave.
m) is generated. The fourth harmonic generated by the wavelength converter 843 passes through the condenser lens 847 and enters the right wavelength converter (non-linear optical crystal) 844, where the second harmonic is further generated, and the incident wave ( Twice the frequency 4ω of the fourth harmonic, ie, eight times the frequency 8 of the fundamental wave.
An eighth harmonic having ω (wavelength 193 nm) is generated.

In this embodiment, as the nonlinear optical crystal used for the wavelength conversion, for example, a wavelength conversion section 842
The LBO crystal is used as the wavelength conversion crystal for converting the fundamental wave into the second harmonic in the above, the BBO crystal is used as the wavelength conversion crystal for converting the second harmonic to the fourth harmonic in the wavelength converter 843, and the LBO crystal is used in the wavelength converter 844.
An SBBO crystal is used as a wavelength conversion crystal from a harmonic to an eighth harmonic.

In the present embodiment, the fundamental wave (wavelength 1.54
4 μm) → 2nd harmonic (wavelength 772 nm) → 4th harmonic (wavelength 3
Although the case where wavelength conversion is performed in the order of 86 nm) to 8th harmonic (wavelength 193 nm) is shown, this corresponds to a configuration in which a plurality of the wavelength conversion units of FIG. Therefore, a configuration obtained by parallelizing a plurality of the other wavelength conversion units shown in FIGS. 11B to 11D in the same manner as in the present embodiment can also be configured in the same manner as the present embodiment. . Similarly, a plurality of the wavelength converters shown in FIGS. 13 and 14 may be configured in parallel.

Next, with reference to FIG. 16, a description will be given of a second example of the present embodiment regarding the coupling section between the optical amplifier and the wavelength conversion section. In this embodiment, the wavelength converter shown in FIG. 15 has a parallel configuration of five optical paths, and the output end of the fiber optical amplifier is divided into five to form five fiber bundles (output groups). Things. In this division, the output end of the fiber optical amplifier is not equally divided into five, and the output end 850 of a part (one fiber bundle in FIG. 15) of the five fiber bundles (output group) is a single or a small number of fiber optical amplifiers. Configure and others (Fig. 1
The four fiber bundle output terminals 851 are bundled with a plurality of fiber optical amplifiers equally divided so that the number of fiber optical amplifiers is the same.

These output lights are supplied to wavelength converters 852 to 852 provided for each output group (fiber bundle).
At 57, the light is converted into ultraviolet light of a predetermined wavelength and supplied to, for example, an exposure apparatus. Each of the three-stage wavelength converters 852 to 854 is composed of a plurality of (five) fiber bundles and the same number of wavelength converters.
Condensing optical elements 855 to 8 arranged on the incident side of
57 also includes the same number of condenser lenses as the fiber bundle.

Here, when the ultraviolet laser device according to this embodiment is applied to an exposure apparatus (FIG. 19 or FIG. 20), the fundamental waves generated from the output ends 851 of the four fiber bundles are converted by the wavelength converters (852 to 857). ), The wavelength is converted to ultraviolet light, and this ultraviolet light is irradiated on the reticle as illumination light for exposure through an illumination optical system. That is, the four fiber bundles are used as light sources for exposure. On the other hand, the light output generated from the output end 850 of the fiber bundle composed of a single or a small number of fiber optical amplifiers and converted into ultraviolet light is guided to an alignment system or a monitor system provided in the exposure apparatus. . That is, one fiber bundle (850) is used as an alignment light source or the like. The wavelength-converted ultraviolet light generated from the fiber bundle output end 850 is, for example, 3
The light is transmitted to an alignment system or the like by an undoped fiber coupled to the wavelength conversion unit 854 of the stage.

In FIG. 16, the fundamental wave generated from the output end 851 of the four fiber bundles is converted to ultraviolet light and guided to the illumination optical system. However, the number of fiber bundles is one. May also be plural. Although one fiber bundle is used for alignment and monitoring, the number may be plural, and light emitted from the plural fiber bundles may be guided to different optical systems.

In this example, the light source for exposure and the light source for alignment are used.
Or, the light source used for monitoring or the like is the same, and the illumination light for exposure and the illumination light for alignment are obtained by splitting, amplifying, and wavelength-converting the output light of the same single-wavelength oscillation laser, and have the same wavelength. Ultraviolet light can be used.
For this reason, alignment or various types of monitoring can be performed through an optical system such as an illumination optical system or a projection optical system of the exposure apparatus.

Accordingly, the design of the alignment optical system and the like is facilitated, and the configuration can be greatly simplified, or there is no need to provide a separate arrangement, and the exposure apparatus can be easily constructed. Since the irradiation of the exposure illumination light and the irradiation of the alignment illumination light or the like may not be performed simultaneously, for example, a shutter may be provided in the illumination light path, or a channel for distributing the pulse light by the TDM 23 may be selected. It is preferable to control the timing of the irradiation independently.

Further, in order to measure the focal position, projection magnification, aberration, telecentricity, etc. of the projection optical system, the aforementioned ultraviolet light for alignment and monitor can be used, and the measurement accuracy is improved. It becomes possible. The image forming plane of the projection optical system and the photosensitive substrate (wafer)
In the case of focusing, the use of light having the same wavelength as the exposure wavelength and focusing through a projection optical system can simultaneously improve the positioning accuracy.

By the way, according to the configuration of the present embodiment (FIGS. 15 and 16) as described above, the fiber output of the fiber optical amplifier is divided into a plurality of groups, and the input light to the nonlinear optical crystal is divided. Thereby, the incident power to the nonlinear optical crystal can be effectively reduced. Therefore, it is possible to solve problems such as output reduction and optical damage caused by light absorption and thermal effects in the nonlinear optical crystal. Note that the number of divisions (the number of fiber bundles) at the output end of the fiber optical amplifier is not limited to four or five, but may be two or more.

Next, in the ultraviolet light generating apparatus according to the present invention, a coupling portion between an optical amplifier and a wavelength converter will be described.
It will be described as. Here, the output end of the optical amplifier is formed by bundling the output end of the fiber optical amplifier as described in the first and second embodiments. At this time, the cladding diameter of each fiber optical amplifier was 125 μm.
Therefore, the diameter of the bundle at the output end where the 128 bundles are bundled can be set to about 2 mm or less.

Here, the number and shape of the bundles can be determined according to the configuration of the wavelength converter and the required shape of the light source. For example, in the first and second embodiments, a bundle having one circular cross section is used. (114,
29, 501, 601, 701, etc.). At this time, if the output end of the fiber optical amplifier is formed on a flat surface as shown in FIG. 9 or FIG. 10, for example, the output end of the fiber bundle and the first-stage wavelength converter (non-linear optical A condensing lens (for example, the condensing lens 845 in FIG. 15) is provided between the non-linear optical crystal and the non-linear optical crystal to effectively output light from the fiber optical amplifier. Can be incident.

FIG. 17 shows another embodiment of the connecting portion according to the present invention. In FIG. 17, a fundamental wave is emitted from a fiber bundle output end 901 in which the emission ends of a plurality of fiber optical amplifiers are bundled, and a lens 902 is arranged for each fiber optical amplifier. Eye wavelength converter (non-linear optical crystal) 9
03 (for example, 50 in the fourth embodiment (FIG. 11)).
2, 507, 518, 533, etc.). In this embodiment, an example will be described in which the diameter of the entire fiber bundle is 2 mm, the mode diameter of each fiber optical amplifier constituting the fiber bundle is 20 μm, and light is condensed on the first-stage wavelength conversion unit 903 by an individual lens 902. . In addition,
First-stage wavelength converter 903 and second-stage wavelength converter 906
A pair of lenses 904 and 905 are disposed between the light source and the wavelength conversion unit 903 so that light emitted from the wavelength conversion unit 903 enters the wavelength conversion unit 906 under the same conditions as when the light enters the wavelength conversion unit 903. ing.

In such an embodiment, the condensing lens is set so that each beam diameter in the nonlinear optical crystal has a size (for example, about 200 μm in this embodiment) desired to obtain the optimum harmonic conversion efficiency. A magnification of 902 (for example, about 10 times in this embodiment) is selected. Since each fiber output is condensed by an individual lens 902, the size (cross-sectional area) of the total luminous flux in the nonlinear crystal collected from all the fibers in the fiber bundle depends on the magnification of the condensing lens. Regardless of the diameter, the diameter is about the diameter of the fiber bundle itself. Therefore, the required size (cross section) of the wavelength conversion crystal
Is about the diameter of a fiber bundle, so that a small wavelength conversion crystal of about several mm square can be used, which is economical. Instead of providing the lens 902, the fiber output end face may be directly processed into a spherical or aspherical lens shape to have the function of a condensing optical element.

FIG. 18 shows another embodiment of the fiber output end in the coupling section between the optical amplifier and the wavelength conversion section.
In the embodiment shown in FIGS. 18A and 18C, the condensing lens 902 shown in FIG. 17 is formed at the output end of each fiber 452, and this is bundled for each output group. An example is shown. In this example, fiber 4
A condensing optical element 453 is formed at the output end of each of the 52. The window member 433 provided at the fiber output end already described with reference to FIG. It has the function of a condensing optical element. With this configuration, it is possible to provide a light collecting function similar to that of FIG. 17 and to suppress damage to the fiber output end face.

FIG. 18B shows a plurality of fibers 4.
This is an embodiment in which a light-collecting optical element 463 is provided for each output group in which 62 are bundled. In this example, for example, the condenser lens 845 shown in FIG. 15 is formed at the output end of the fiber bundle, and the window member 443 already described with reference to FIG. This has a function of a condensing optical element.

Instead of processing the fiber end or the output surface of the window member into a spherical or aspherical lens shape, the fiber end is formed by ion exchange such as thermal ion exchange or electrolytic ion exchange. Alternatively, when a glass window is used as a window member, the glass composition at the end of the glass window is partially changed by ion exchange, thereby giving a refractive index distribution equivalent to that of a lens, thereby providing a condensing optical function. It may be. In addition, FIG.
In (c), the diameters of the cores 451 and 461 in the fiber are not enlarged, but this enlargement of the core diameter can be used together.

The light condensing on the second and subsequent wavelength conversion units (non-linear optical crystals) can be output by individual lenses for each fiber or each bundle as in the case of the first stage. However, the present embodiment describes a case where all outputs of the fiber bundle are condensed by a common set or one lens. By using a common lens in this way, the number of lenses used is reduced,
It is economical because the alignment of the lens becomes easy.

Since the output end of the wavelength conversion crystal (non-linear optical crystal) is located within the Rayleigh length of the beam condensed by the wavelength conversion crystal, the beam emitted from the wavelength conversion crystal is output from the wavelength conversion crystal. It becomes almost parallel light at the end. In the present embodiment (FIG. 17), this emission beam is
4 and 905 show the case where light is condensed on the second-stage wavelength conversion crystal 906. Here, the focal length of the lens pair can be set to a magnification that provides a desirable beam diameter for obtaining optimum conversion efficiency in the second-stage wavelength converter 906. The condensing optical elements (for example, 505 and 506 shown in FIG. 11A) for condensing the fundamental wave or its harmonics on the wavelength conversion crystal shown in FIGS. 11, 13 and 14 are one lens. However, it is also possible to use a single lens as in the present embodiment.

As described above, the fundamental wave generator (laser light generator and optical amplifier) is constituted by the structure shown in the first to third embodiments, and the wavelength converter is constituted by the structure shown in the fourth to seventh embodiments. In addition, by configuring the coupling section between the optical amplifier and the wavelength conversion section with the configuration shown in the eighth embodiment, it is possible to obtain an ultraviolet light output with an output wavelength of 157 nm, 193 nm or the like. These wavelengths are the same as the oscillation wavelengths of the F ₂ laser and the ArF excimer laser, respectively.

In addition, the ultraviolet output light obtained in this manner is a pulse light emitted at intervals of about 3 ns when the fundamental wave generation unit according to the first embodiment is used, for example. The output light does not interfere with each other even though it is a single-wavelength ultraviolet light having a very narrow band without overlapping. Further, for example, in the case of using the fundamental wave generation unit according to the second embodiment, the obtained ultraviolet output light is pulsed light that is emitted at equal intervals of about 78 ns, and thus does not overlap with each other in time. Even though the single-wavelength ultraviolet light has a very narrow band, the individual output lights do not interfere with each other.

Further, in a solid-state ultraviolet laser array as disclosed in, for example, JP-A-8-334803, a wavelength converter is provided for each parallelized fundamental wave laser (for each laser element). Necessary,
According to the present embodiment, since the fiber bundle diameter of the fundamental wave output is 2 mm or less even when all the channels are combined, it is possible to perform the wavelength conversion of all the channels with only one set of the wavelength converters. In addition, since the output end is a flexible fiber, it is possible to arrange the wavelength converter and other components such as a single-wavelength oscillation laser, a splitter, and a time division optical branching unit separately. Extremely high degree of freedom. Therefore, according to the present invention, it is possible to provide an inexpensive and compact ultraviolet laser device having a single wavelength and low spatial coherence.

Next, a ninth embodiment of the ultraviolet laser device according to the present invention will be described. The ultraviolet laser device according to the present embodiment is characterized in that the ultraviolet laser device as already described in the first to eighth embodiments is a light source for an exposure device.

An embodiment of an exposure apparatus using the ultraviolet laser device according to the present invention will be described below with reference to FIG. The exposure apparatus used in the optical lithography process is in principle the same as photolithography, in which a device pattern precisely drawn on a photomask (reticle) is converted to a semiconductor wafer or glass substrate coated with photoresist. It is optically projected onto and transferred. The ultraviolet laser device 1261 according to the present invention includes an illumination optical system 1262, a projection optical system 12
65 and the like are provided integrally with the entire exposure apparatus.
At this time, the ultraviolet laser device 1261 may be fixed to a mount supporting the illumination optical system 1262, or the ultraviolet laser device 1261 may be fixed to the mount alone. However, it is preferable that a power supply and the like connected to the ultraviolet laser device 1261 be separately provided.

The ultraviolet laser device 1261 is divided into a first portion having a laser beam generator and an optical amplifier, and a second portion having a wavelength converter.
The first portion may be fixed to a gantry different from the gantry while being fixed to the gantry integrally with the gantry. Further, all of the ultraviolet laser device 1261 may be arranged in a chamber accommodating the exposure apparatus main body, or a part of the ultraviolet laser device 1261, for example, a wavelength conversion unit is arranged in the chamber, and the remaining part is provided with the chamber You may make it arrange | position to the outside integrally. The control system of the ultraviolet laser device 1261 may be housed in a control rack separately from the chamber, or a display unit (display), switches, and the like may be disposed outside the chamber integrally with the chamber, and the rest may be provided. You may arrange | position in a chamber.

The ultraviolet light having a narrow band and low spatial coherence according to the present invention is applied to the illumination optical system 1262.
Thus, the illuminance distribution is enlarged and projected so that the required illuminance distribution on the required projection plane becomes uniform, and is irradiated onto a quartz mask (quartz reticle) 1263 on which a circuit pattern of an integrated circuit is accurately drawn. The circuit pattern of the reticle 1263 corresponds to the projection optical system 1
The circuit pattern is projected on a semiconductor wafer (for example, a silicon wafer) 1266 coated with a photoresist after being reduced at a predetermined reduction magnification by 265, and the circuit pattern is imaged and transferred on the wafer.

The illumination optical system 1262 includes a reticle 1263
A field stop that is arranged in a plane substantially conjugate to the pattern plane of the reticle 1263 and that defines an illumination area on the reticle 1263. And a condenser lens that irradiates the reticle 1263 with ultraviolet light emitted from the aperture stop. At this time, in order to change the distribution of the amount of ultraviolet light on the predetermined surface, a plurality of aperture stops having at least one of shapes and sizes different from each other are provided on the turret, and a plurality of aperture stops selected according to the pattern of the reticle 1263 are provided. One of the aperture stops may be arranged in the optical path of the illumination optical system 1262.

Also, an optical integrator (homogenizer) may be arranged between the wavelength converter of the ultraviolet laser device 1261 and the field stop. And are arranged so as to have a relationship of almost Fourier transform,
When a rod integrator is used, the rod integrator may be arranged such that its emission surface is substantially conjugate with the pattern surface of the reticle 1263.

As the exposure start shutter of the exposure apparatus, the electro-optic modulator or the acousto-optic modulator (12, 22, 32) described in the first to third embodiments can be used. The electro-optic or acousto-optic modulator is switched from an off state, ie, a state in which no pulse is generated (internal loss is large), to an on state, ie, a state in which a pulse is generated (internal loss is reduced in a pulse). Start exposure.

In the exposure apparatus having the ultraviolet laser device 1261, continuous light may be output from the single-wavelength oscillation laser constituting the ultraviolet laser device 1261, or the single-wavelength oscillation laser may be pulse-output. May be. In particular, in the latter case, the reticle 1263 and the semiconductor wafer 126 are combined by using both the current control of the single-wavelength oscillation laser and the control of the above-described electro-optic or acousto-optic modulator.
The output interval of the ultraviolet light (pulse light) applied to 6, and the start and stop of the output may be controlled.

Further, the ultraviolet laser device 12 of this embodiment
In the exposure apparatus having 61, it is not necessary to control the integrated amount of ultraviolet light on the wafer 1266 using a mechanical shutter, but for example, the output (power, center wavelength, wavelength width, etc.) of the ultraviolet laser device 1261 is controlled. When oscillating ultraviolet light for stabilization, to prevent the ultraviolet light from reaching the wafer 1266 and exposing the photoresist,
A shutter may be provided in the illumination optical path between the ultraviolet laser device 1261 and the wafer 1266, or the stage 1267 may be driven to retract the wafer 1266 from the ultraviolet light irradiation area.

The semiconductor wafer 1266 is driven by the drive mechanism 12
The circuit pattern is transferred to a different position on the semiconductor wafer by being placed on a stage 1267 having a 69 and moving the stage each time one exposure is completed. Such a stage driving and exposure method is called a step-and-repeat method. In addition to the stage driving and exposure methods, there is a step-and-scan method in which a driving mechanism is also provided on a support member 1264 that supports the reticle 1263, and scanning exposure is performed by synchronously moving the reticle and the semiconductor wafer. The ultraviolet laser device of the present invention can be applied to this method.

In an exposure apparatus that performs exposure with ultraviolet light, such as an exposure apparatus using an ultraviolet laser apparatus according to the present invention, the illumination optical system 1262 and the projection optical system 1265 are generally composed of an all-quartz lens without color correction. It is. In particular, when the wavelength of the ultraviolet light is 200 nm or less, the projection optical system 12
At least one of the plurality of refractive optical elements constituting 65 may be made of fluorite, or a catadioptric optical system combining at least one reflective optical element (concave mirror, mirror, etc.) and a refractive optical element. May be used.

As described above, the exposure apparatus using the ultraviolet laser apparatus according to the present invention is smaller than other conventional methods (exposure apparatus using excimer laser or solid-state laser), and each element is Since it is configured by fiber connection, there is a high degree of freedom in the arrangement of each unit constituting the apparatus. FIG. 20 shows another embodiment utilizing the characteristics of the ultraviolet laser device according to the present invention.

In this embodiment, the components of the laser beam generator (single-wavelength laser, optical branching means, etc.) and the optical amplifier of the laser apparatus described in the first to third embodiments and the fourth to seventh embodiments are described.
And the wavelength conversion section described in (1) is separately disposed to constitute an exposure apparatus. That is, while the wavelength conversion unit 1272 is mounted on the main body of the exposure apparatus, another part (laser light generation unit, optical amplifier, etc.) 1271 of the ultraviolet laser apparatus is separately provided outside the main body of the exposure apparatus, and Are connected by a connection fiber 1273 to form an ultraviolet laser device. Here, the connection fiber 1273 may be a fiber of the fiber optical amplifier itself (for example, the fiber bundle 114 in the first embodiment), an undoped fiber, or a combination thereof. Note that the portion of the exposure machine main body other than the ultraviolet laser device can be configured using the same device as that in FIG.

With this configuration, the main components that generate heat, such as the semiconductor laser for excitation of the fiber optical amplifier, the power supply for driving the semiconductor laser, and the temperature controller, are disposed outside the exposure apparatus body. Can be. Therefore, it is possible to suppress a problem caused by heat such that the alignment of the optical axis is out of order due to the influence of heat generated from the ultraviolet laser device as the exposure light source in the exposure device main body.

By the way, as shown in FIG.
The reticle stage 1264 holding the 263 is configured to be movable in the X and Y directions by the driving mechanism 1268 and to be able to rotate minutely. Also, the wafer stage 1
A reference mark plate FM is provided on the reference numeral 267, and this reference mark plate is used for, for example, baseline measurement described later. Further, in this example, an alignment system 1280 for detecting an alignment mark on the reticle 1263 and an off-axis alignment system 1281 provided separately from the projection optical system 1265 are provided.

The alignment system 1280 supplies the illumination light for exposure or the illumination light in the same wavelength range as the reticle 1263.
The above-mentioned alignment mark and the reference mark on the reference mark plate FM are radiated through the projection optical system 1265, and the light generated from both marks is received by an image pickup device (CCD) to detect the positional shift. Reticle 1
It is used for alignment of H.263, baseline measurement of the alignment system 1281, and the like.

Off-Axis Alignment System 128
1 irradiates an alignment mark on the semiconductor wafer 1266 with white light (broadband light) having a wavelength width of, for example, about 550 to 750 nm, and converts an image of an index mark and an image of the alignment mark provided therein into an image sensor. An image is formed on a (CCD) to detect a positional shift between the two marks.

Note that alignment systems 1280 and 1281
By detecting the reference marks on the reference mark plate FM, the base line amount of the alignment system 1281 can be measured from the detection result. Although the baseline measurement is performed before the exposure of the semiconductor wafer is started, the baseline measurement may be performed every time the semiconductor wafer is exchanged, or the base line measurement may be performed once in the exposure operation of a plurality of semiconductor wafers. Line measurement may be performed. However, baseline measurement is always performed after reticle replacement.

In the present example, the wavelength converter shown in FIG. 16 is used as the wavelength converter connected to the ultraviolet laser device (fundamental wave generator) 1271. That is, the wavelength converter 1272 into which the fundamental wave generated from the four fiber bundle output terminals 851 is incident and the wavelength converter 1279 into which the fundamental wave generated from the fiber bundle output terminal 850 is incident are separated. The wavelength conversion unit 1279 is provided integrally with a gantry holding the alignment system 1280. The wavelength conversion unit 1279 is provided integrally with a gantry holding the illumination optical system 1262. At this time, the connection fiber 1278 is coupled to the fiber bundle output end 850 to guide the fundamental wave to the wavelength converter 1279. Accordingly, it is not necessary to separately prepare a light source for the alignment system 1280, and the reference mark can be detected using illumination light having the same wavelength as the illumination light for exposure, thereby enabling highly accurate mark detection.

In this embodiment, the illumination light having the same wavelength as the exposure illumination light is guided to the alignment system 1280.
A wavelength longer than the wavelength (for example, 193 nm) of the exposure illumination light may be guided to the alignment system 1280 or 1281 or the like. That is, of the three stages of wavelength converters shown in FIG. 16, for example, the pulse light emitted from the second stage wavelength converter 853 may be guided to the alignment system by the connection fiber. In addition, a part of the pulse light emitted from the first-stage wavelength conversion unit 852 is branched, and the remaining pulse light is wavelength-converted by the second-stage wavelength conversion unit 853.
Two pulse lights having different wavelengths respectively emitted from the two wavelength converters 852 and 853 may be guided to the alignment system.

The exposure apparatus shown in FIG. 20 has a single-wavelength oscillation laser,
The oscillation wavelength of the DFB semiconductor laser, that is, the reticle 1263 is adjusted by adjusting the temperature using a temperature controller (for example, a Peltier element) provided on a heat sink on which the B semiconductor laser (such as 11 in FIG. 1) is mounted. Is provided with a wavelength control device 1274 for controlling the wavelength of the ultraviolet laser light (exposure illumination light) applied to the substrate. Wavelength control device 127
Reference numeral 4 controls the temperature of the DFB semiconductor laser in units of 0.001 ° C. to stabilize the center wavelength of the ultraviolet laser light and adjust the optical characteristics (aberration, focal position, projection magnification, etc.) of the projection optical system 1265. And so on. Thereby, the wavelength stability of the ultraviolet laser light during the exposure operation of the semiconductor wafer can be improved, and the irradiation of the ultraviolet laser light, and the optical characteristics of the projection optical system 1265 that fluctuate due to a change in the atmospheric pressure and the like can be improved. It can be easily adjusted.

Further, the exposure apparatus shown in FIG. 20 has a light modulation element (FIG. 1) for converting continuous light generated from a single-wavelength oscillation laser (such as a DFB semiconductor laser) into pulse light in a fundamental wave generation section 1271. A pulse control unit 1275 for applying a drive voltage pulse to the semiconductor wafer 1266, and a pulse necessary to expose the photoresist during circuit pattern transfer according to the sensitivity characteristics of the photoresist applied to the semiconductor wafer 1266. The exposure control unit 1276 controls the oscillation timing and the magnitude of the control pulse output from the pulse control unit 1275 in accordance with the number of pulses, and the control unit 1277 controls the entire exposure apparatus. Are provided.

Here, the pulse control unit 1275 controls the current of the single-wavelength oscillation laser (11 or the like) in the fundamental wave generation unit 1271 or the voltage applied to the light modulation element 12 to control the single-wavelength oscillation. The laser can also be pulsed. That is, the pulse control unit 12
By controlling the output of the current or the voltage by 75, the single-wavelength oscillation laser can switch between continuous light and pulsed light and output it. In this embodiment, the pulse control unit 1
275 causes the single-wavelength laser to oscillate in pulses, and cuts out only a part of the oscillated pulse light (pulse width: about 10 to 20 ns) by the control of the light modulation element, that is, a pulse having a pulse width of 1 ns Modulates into light. This makes it possible to easily generate pulsed light having a high extinction ratio as compared to a case where continuous light is converted into pulsed light using only the light modulation element.
The exposure control unit 1276 makes it possible to more easily control the pulse output interval, the start and stop of the pulse output, and the like.

The pulse control section 1275 not only switches between pulse oscillation and continuous oscillation of the single-wavelength oscillation laser,
In addition to controlling the pulse output interval and pulse width, the oscillation control of the single-wavelength oscillation laser and the control of the magnitude of the voltage pulse applied to the light modulation element are performed so as to compensate for the fluctuation in the output of the pulse light. Do at least one of This makes it possible to compensate for the output fluctuation of the pulse light that occurs when the oscillation interval of the pulse light is changed or when the oscillation of the pulse light is restarted. That is, the output (intensity) of each pulse can be always maintained at a substantially constant value.

Further, the pulse control unit 1275 adjusts at least one gain of a plurality of fiber optical amplifiers (13, 18, 19, etc. in FIG. 1) arranged in series in the fundamental wave generation unit 1271. The intensity of the pulse light on the semiconductor wafer can be controlled only by adjusting the gain or by using the control of the light modulation element described above. Note that it is also possible to control at least one gain of a fiber optical amplifier provided in parallel corresponding to the plurality of channels divided in parallel by the optical branching device.

The exposure control unit 1276 outputs the fundamental wave output from the fundamental wave generation unit 1271 or the wavelength conversion unit 1227.
72 output from the ultraviolet light or the wavelength converter 127
2, a pulse light output from, for example, the first-stage or second-stage nonlinear optical crystal is detected, and the pulse control unit 1275 is controlled based on the detected value (including intensity, wavelength, and wavelength width). By controlling, the oscillation interval of the pulse light, the start and stop of the oscillation, the intensity of the pulse light, and the like are adjusted. Further, the detected value is also input to the wavelength controller 1274, and the wavelength controller 1274
Performs the temperature control of the single-wavelength oscillation laser based on the detected value, and adjusts the center wavelength and the wavelength width of the exposure illumination light (ultraviolet laser light).

The controller 1277 exposes information (not shown) of a reading device (not shown) for an identification symbol (bar code or the like) attached to a semiconductor wafer or a cassette holding the semiconductor wafer, or exposes information relating to the sensitivity characteristics of the photoresist input by an operator. The exposure control unit 1276 calculates the number of exposure pulses required for pattern transfer based on the input information. Further, the exposure control unit 1276 controls the trigger pulse control unit 1275 based on the number of exposure pulses and the intensity of the pulse light determined according to the number of exposure pulses, and oscillates the control pulse applied to the light modulation element and the magnitude of the control pulse. Adjust the length. This controls the start and end of the exposure, and the intensity of the pulse light irradiated on the semiconductor wafer 1266, and the integrated light amount given to the photoresist by the irradiation of the plurality of pulse lights is adjusted to an appropriate exposure amount corresponding to the sensitivity. Controlled.

The exposure control unit 1276 sends a command to the pulse control unit 1275 to control the current of the single-wavelength oscillating laser, so that the exposure control is performed only by the current control or in combination with the control of the light modulation element. The start and end of (pulse output) can be controlled.

Here, when the laser device shown in FIG. 1 or FIG. 2 is used as the fundamental wave generator 1271 in this example, one pulse light cut out by the light modulation element is divided into a plurality (128). However, in this example, the divided 12
Eight pulse lights may be used as one pulse to perform exposure amount control in units of this pulse, or the divided 128 pulse lights may be used as one pulse to perform exposure amount control. Good. When the latter exposure amount control is performed, the gain of the fiber optical amplifier in the fundamental wave generation unit 1271 is adjusted instead of the control of the light modulation element by the pulse control unit 1275, and the pulse on the semiconductor wafer is adjusted. The light intensity may be controlled, or the two controls may be used in combination.

The exposure apparatus shown in FIG. 20 is capable of selectively exposing a semiconductor wafer by switching between a step-and-repeat method and a step-and-scan method. In the step-and-repeat method, the illumination optical system 126 is configured such that the entire circuit pattern on the reticle 1263 is irradiated with the illumination light for exposure.
The field stop (reticle blind) in 2 is driven to adjust the size of the opening and the like. On the other hand, in the step-and-scan method, the irradiation area of the exposure illumination light within the circular projection field of view of the projection optical system 1265 is limited to a rectangular slit shape extending along a direction orthogonal to the scanning direction of the reticle 1263. Adjust the aperture of the field stop. Therefore,
In the step-and-scan method, the reticle 1263
Since only a part of the upper circuit pattern is illuminated, the entire circuit pattern is scanned and exposed on a semiconductor wafer, so that the projection is synchronized with the relative movement of the reticle 1263 with respect to the exposure illumination light. The semiconductor wafer 1266 is moved relative to the exposure illumination light at a speed ratio corresponding to the projection magnification of the optical system 1265.

In the exposure control during the scanning exposure, at least one of the pulse repetition frequency f defined by the light modulation element and the inter-channel delay time defined by the TDM 23 shown in FIG. 2 is adjusted. Then, a plurality of pulse lights are oscillated at equal time intervals from the fundamental wave generator 1271 during the scanning exposure. Further, in accordance with the sensitivity characteristics of the photoresist, the intensity of the pulse light on the semiconductor wafer, the scanning speed of the semiconductor wafer, the oscillation interval (frequency) of the pulse light, and the pulse light in the scanning direction of the semiconductor wafer (that is, the irradiation area thereof) ) Is adjusted, and the integrated light amount of the plurality of pulsed lights irradiated while each point on the semiconductor wafer crosses the irradiation area is controlled to an appropriate exposure amount. At this time, in consideration of throughput, other control parameters, that is, pulse light intensity, oscillation frequency, and irradiation area, are controlled in the exposure amount control so that the scanning speed of the semiconductor wafer is almost maintained at the maximum speed of the wafer stage 1267. It is preferable to adjust at least one of the widths.

When scanning exposure is performed using the laser apparatus shown in FIG. 1 or FIG. 2, in the exposure amount control, the 128 divided pulsed lights are oscillated at equal time intervals as one pulse each as described above. Preferably. However, the oscillation interval of the divided 128 pulse lights is adjusted according to the scanning speed of the semiconductor wafer, and the 128 pulse lights can be regarded as one pulse, that is, the 128 pulse lights are irradiated. If the distance that the semiconductor wafer moves during this time does not cause a decrease in the exposure control accuracy,
The exposure amount control may be performed with 28 pulsed lights as one pulse.

In the above description of each embodiment of the present invention, a configuration example of an ultraviolet laser device that outputs the same output wavelength of 193 nm or 157 nm as an ArF excimer laser or an F ₂ laser has been described. However, the present invention is not limited to a laser device having this wavelength, and the same output wavelength as that of a KrF excimer laser, for example, 248 nm can be generated by appropriately selecting the configuration of the laser light generator, optical amplifier, and wavelength converter. It is also possible to provide an ultraviolet laser device.

For example, an yttria (Yb) -doped fiber laser or a semiconductor laser oscillating at 992 nm is used as a single-wavelength oscillation laser in a laser light generator, and an ytterbium-doped fiber optical amplifier is used as a fiber optical amplifier. The second harmonic (wavelength 496 nm) is generated using the LBO crystal as the output of the fiber optical amplifier.
By constructing a fourth harmonic generation optical path for generating the fourth harmonic (wavelength: 248 nm) ultraviolet light using an O crystal, an ultraviolet laser device that generates the same 248 nm ultraviolet light as the KrF excimer laser can be provided. Can be provided.

It is preferable that the surface of the fiber (including the fiber optical amplifier and the like) used in the above-described embodiment is covered with Teflon. It is desirable that the coating with Teflon be performed on all the fibers. In particular, the fibers disposed in the chamber accommodating the exposure apparatus main body are coated with Teflon. This is because foreign matter (including fibers and the like) generated from the fiber may become a substance that contaminates the exposure apparatus, and constitutes an illumination optical system, a projection optical system, an alignment optical system, and the like generated due to the contaminant. To prevent fogging of optical elements, fluctuations in transmittance (reflectance) and optical characteristics (including aberrations) of these optical systems, or fluctuations in illuminance on a reticle or a semiconductor wafer and distribution thereof. It becomes possible. Instead of coating with Teflon, the fibers arranged in the chamber may be collectively stored in a stainless steel housing.

In the semiconductor device, a step of designing its function and performance, a step of manufacturing a reticle based on this design step, a step of manufacturing a wafer from a silicon material, and a step of forming a reticle pattern on the wafer using the above-described exposure apparatus. , A device assembling step (including a dicing step, a bonding step, and a package step), and an inspection step. In addition, the above-described exposure apparatus can be used not only for manufacturing semiconductor elements, but also, for example, for a liquid crystal display, an image sensor (eg, a CCD).
Etc.), a device such as a thin-film magnetic head, or a reticle.

Further, an illumination optical system composed of a plurality of optical elements and a projection optical system are incorporated into the exposure apparatus main body to perform optical adjustment thereof, and a reticle stage or a wafer stage composed of a large number of mechanical parts is mounted on the exposure apparatus main body. The exposure apparatus according to the present embodiment can be manufactured by attaching wires and pipes, and performing overall adjustment (electrical adjustment, operation confirmation, and the like).

In the above-described exposure apparatus, the ultraviolet laser apparatus 1261 is attached to the exposure apparatus main body, or a part of the ultraviolet laser apparatus 1261 (such as a laser beam generating section and an optical amplifier) and the main body are disposed outside the exposure apparatus main body. A fiber is connected to a wavelength conversion unit disposed in the inside, and an optical axis alignment between the ultraviolet laser device 1261 (wavelength conversion unit) and the illumination optical system 1262 is performed. It is desirable that the exposure apparatus be manufactured in a clean room in which the temperature, the degree of cleanliness, and the like are controlled.

In the ninth embodiment, the laser apparatus according to the present invention is applied to an exposure apparatus. However, in order to cut a part (such as a fuse) of a circuit pattern formed on a wafer, for example, The laser device according to the present invention can be used for a laser repair device or the like to be used. Further, the laser device according to the present invention can be applied to an inspection device using visible light or infrared light. In this case, it is not necessary to incorporate the wavelength converter described in the fourth to seventh embodiments into the laser device. That is,
The present invention is effective not only for an ultraviolet laser device but also for a laser device that generates a fundamental wave in the visible or infrared region and has no wavelength conversion unit.

[0238]

As described above, according to the present invention,
It is possible to provide an ultraviolet laser device that is compact, has a high degree of freedom in equipment arrangement, is easy to maintain, hardly causes damage to the nonlinear optical crystal, and generates ultraviolet light with low spatial coherence.

[Brief description of the drawings]

FIG. 1 is an explanatory diagram showing a configuration of a laser light generator and an optical amplifier according to a first embodiment of an ultraviolet laser device according to the present invention.

FIG. 2 is an explanatory diagram showing a configuration of a laser light generator and an optical amplifier according to a second embodiment of the ultraviolet laser device according to the present invention.

FIG. 3 is an explanatory diagram showing a configuration of a laser light generator and an optical amplifier according to a third embodiment of the ultraviolet laser device according to the present invention.

FIG. 4 is an explanatory diagram showing a configuration of an optical amplifier according to another embodiment of the ultraviolet laser device according to the present invention.

FIG. 5 is a cross-sectional view of a double clad fiber optical amplifier.

FIG. 6 is a characteristic diagram showing a relationship between wavelength and gain by an element doped into an erbium-doped fiber optical amplifier.

FIG. 7 is a characteristic diagram showing a change in gain with respect to pumping intensity in a fiber optical amplifier in which erbium and yttrium are co-doped.

FIG. 8 is a configuration diagram showing a configuration of a fiber output control unit of the ultraviolet laser device according to the present invention.

FIG. 9 is a side view illustrating an enlarged state of a fiber core at an output end of the fiber optical amplifier.

FIG. 10 is a side view showing an example of an output end of the fiber optical amplifier.

FIG. 11 is an explanatory diagram illustrating a configuration of a wavelength conversion unit according to a fourth embodiment of the ultraviolet laser device according to the present invention.

FIG. 12 is a table showing the conversion efficiency of the wavelength converter according to the present invention.

FIG. 13 is an explanatory diagram illustrating a configuration of a wavelength conversion unit according to a fifth embodiment of the ultraviolet laser device according to the present invention.

FIG. 14 is an explanatory diagram illustrating a configuration of a wavelength conversion unit of a sixth embodiment of the ultraviolet laser device according to the present invention.

FIG. 15 is an explanatory diagram illustrating a configuration of a wavelength conversion unit according to a seventh embodiment of the ultraviolet laser device according to the present invention.

FIG. 16 is an explanatory diagram showing an example of an input section of a wavelength conversion section which is an eighth embodiment of the ultraviolet laser apparatus according to the present invention.

FIG. 17 is an explanatory view showing another embodiment of the input section of the wavelength conversion section of the ultraviolet laser device according to the present invention.

FIG. 18 is an explanatory diagram showing another embodiment of the wavelength converter input section of the ultraviolet laser device according to the present invention.

FIG. 19 is an explanatory view showing a configuration example of an exposure apparatus according to the present invention.

FIG. 20 is an explanatory view showing another configuration example of the exposure apparatus according to the present invention.

[Explanation of symbols]

Reference Signs List 11 light source, single wavelength oscillation laser (DFB semiconductor laser, fiber laser, etc.) 12 optical modulator 14, 16 splitter (optical branching means) 13 fiber optical amplifier 15, 17 fibers having different lengths (delay means, delay fiber) Reference Signs List 18 fiber optical amplifier (first fiber optical amplifier) 19 fiber optical amplifier (second fiber optical amplifier) 114 fiber output end (fiber bundle output end) 21 light source, single-wavelength oscillation laser (DFB semiconductor laser, fiber laser, etc.) 22 Optical modulator 23 Time division optical branching means (TDM, optical branching means, delay means) 24 Fiber optical amplifier (first fiber optical amplifier) 25 Fiber optical amplifier (second fiber optical amplifier) 29 Fiber output end (fiber bundle output end) ) 31 light source, single wavelength emission Vibration laser (DFB semiconductor laser, fiber laser, etc.) 32 Optical modulator 33 Fiber optical amplifier (first fiber optical amplifier) 34 Fiber optical amplifier (second fiber optical amplifier) 41 Fiber optical amplifier (first fiber optical amplifier) 42 Fiber Optical amplifier (second fiber optical amplifier) 405, 406, 407 Fiber output control device 421, 341, 441, 451, 461 Core 423, 434, 444, 454, 464 Fiber output end surface 433, 443 (453, 463) Window member 453, 463 Lens 501 Fiber output end (fiber bundle output end) 502-504, 507, 510, 513, 514, 5,
17, 518, 520, 526, 532, 533, 53
6, 539, 545, 548 Nonlinear optical crystal 601 Fiber output end (fiber bundle output end) 602, 604, 609, 611 Nonlinear optical crystal 701 Fiber output end (fiber bundle output end) 702, 705, 710, 712 Nonlinear optical crystal 841 Fiber output end (fiber bundle output end) 842, 843, 844 Nonlinear optical crystal 901 Fiber output end (fiber bundle output end) 902, 904, 905 Lens 903, 906 Nonlinear optical crystal 1261 Laser device 1262 Illumination optical system 1263 Mask ( (Reticle) 1265 Projection optical system 1266 Wafer 1268, 1269 Driving mechanism (driving device) 1271 Laser device 1272 Wavelength conversion unit 1273 Transmission system (first fiber) 1277 Control device ( Integer unit) 1278 transmission system (second fibers) 1279 wavelength converter 1280,1281 alignment system

──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. ⁷ Identification symbol FI Theme court ゛ (Reference) H01S 3/10 H01S 3/10 Z 3/108 3/108 H01L 21/30 516D (31) Claim number of priority Patent application Hei 10-311147 (32) Priority date October 30, 1998 (Oct. 30, 1998) (33) Priority claiming country Japan (JP) F term (reference) 2H097 AA03 AA11 CA13 GB01 KA03 KA12 KA29 LA10 LA12 2K002 AA04 AB12 CA02 HA18 HA19 HA20 5F046 AA06 AA07 CA04 CA05 CA08 DA02 EB02 FB20 5F072 AB09 AB13 AK06 JJ20 KK12 QQ02 QQ04 RR05 YY09

Claims (71)

[Claims] 1. A laser light generating section having a single-wavelength oscillation laser for generating a single-wavelength laser light within a wavelength range from an infrared region to a visible region, and a laser light generated by the laser light generating portion. An optical amplifier having a fiber optical amplifier for amplification, and a wavelength conversion unit for converting the wavelength of the amplified laser light into ultraviolet light using a nonlinear optical crystal, wherein a single wavelength ultraviolet light is generated. Laser device. 2. The single wavelength oscillation laser according to claim 1, further comprising an oscillation wavelength control means for controlling an oscillation wavelength of the generated laser light to a constant wavelength.
3. The laser device according to claim 1. 3. The laser according to claim 1, wherein the laser device further comprises an optical branching unit that branches a laser beam generated from the single-wavelength oscillation laser into a plurality of laser beams. apparatus. 4. The splitter has a splitter for splitting a plurality of laser beams generated from the single-wavelength oscillation laser in parallel, and fibers having different lengths are provided on the emission side of the splitter. The laser device according to claim 3, wherein: 5. The length of each of the fibers having different lengths is determined so that the delay interval between the parallel-branched laser lights at the output ends of these fibers is substantially constant. The laser device according to claim 4, wherein 6. The respective lengths of the fibers having different lengths are defined as follows: the mutual delay interval of the parallel-branched laser beams at the output ends of these fibers is determined by the repetition frequency of the laser beam incident on the splitter and The laser device according to claim 5, wherein the laser device is determined so as to be a reciprocal of a product of the number of optical paths branched in parallel by the splitter. 7. The laser device according to claim 3, wherein the light splitting means has a time division multiplexer. 8. The output end of the optical amplifier provided on the incident side of the wavelength converter, wherein the core of the fiber output end is formed by expanding in a tapered shape toward the fiber output end face. Item 1
The laser device according to any one of claims 1 to 7. 9. An output terminal of the optical amplifier provided on the incident side of the wavelength conversion unit, further comprising a window member provided at a fiber output terminal and transmitting the laser light amplified by the optical amplifier. The laser device according to any one of claims 1 to 8, wherein: 10. The laser device according to claim 1, wherein the optical amplifier includes an erbium-doped fiber optical amplifier. 11. The laser device according to claim 1, wherein the optical amplifier has a fiber optical amplifier doped with both erbium and yttrium. 12. The optical amplifier according to claim 1, wherein the optical amplifier includes a plurality of fiber optical amplifiers for amplifying the plurality of branched lights branched by the optical branching unit. 3. The laser device according to claim 1. 13. The optical amplifier according to claim 1, wherein the output of the ultraviolet light has a predetermined optical output, or each of the optical outputs amplified by the plurality of fiber optical amplifiers has a predetermined optical output. 13. The apparatus according to claim 12, further comprising fiber output control means for controlling the excitation intensity of each of the plurality of optical amplifiers.
3. The laser device according to claim 1. 14. The output end of the optical amplifier provided on the incident side of the wavelength conversion unit, wherein a plurality of fiber output ends are divided into one or a plurality of output groups, and the output ends are bundled for each output group. The laser device according to claim 12 or 13, wherein: 15. The output group of the optical amplifier divided into the plurality of groups includes: a first output group formed by bundling one or a small number of fiber output ends; and a remaining output group excluding the first output group. Connect the fiber output end to
15. The laser device according to claim 14, comprising a second output group or a plurality of output groups which are substantially equally divided into one or a plurality of output groups and bundled. 16. An output end of the optical amplifier provided on the incident side of the wavelength converter, provided at each fiber output end bundled for each of the output groups, and amplified by the optical amplifier. The laser device according to claim 14, further comprising a window member that transmits the laser light obtained for each of the output groups. 17. The laser device according to claim 14, wherein the wavelength converter is provided for each output group of the optical amplifier. 18. A condensing optical element on an input side of the wavelength conversion unit, for condensing laser light emitted from the optical amplifier to the nonlinear optical crystal for incidence. The laser device according to any one of claims 1 to 17. 19. The laser device according to claim 18, wherein said condensing optical element is provided for each output group of said optical amplifier. 20. The light-collecting optical element according to claim 19, wherein the output end portion bundled for each output group of the optical amplifier is provided as a lens for each output group. Laser device. 21. The laser device according to claim 18, wherein said condensing optical element is provided at each of a plurality of fiber output ends of said optical amplifier. 22. The laser device according to claim 21, wherein the condensing optical element is provided by using a plurality of fiber output ends of the optical amplifier as lenses. 23. The laser light generator, wherein the wavelength is 1.5.
a wavelength of about 1.5 μm, and the wavelength converter outputs the fundamental wave of about 1.5 μm output from the optical amplifier as 8th harmonic or 10th harmonic of ultraviolet light. The laser device according to any one of claims 1 to 22, wherein the laser device is generated. 24. The single wavelength oscillation laser according to claim 1, wherein
a DFB semiconductor laser or a fiber laser having an oscillation wavelength in the range of μm to 1.59 μm, wherein the wavelength conversion unit has a generation wavelength of 189 nm to 199 nm.
24. The laser device according to claim 23, wherein the laser device generates an 8th harmonic within the range. 25. The single-wavelength oscillation laser according to claim 1, wherein
A laser beam having an oscillation wavelength within a range of 4 μm to 1.552 μm; and the wavelength conversion unit generates an eight-fold harmonic within a range of 193 nm to 194 nm whose generation wavelength is substantially the same as the oscillation wavelength of the ArF excimer laser. The laser device according to claim 23, wherein the laser device generates a wave. 26. The wavelength conversion section has a first nonlinear optical crystal that generates an eighth harmonic of the fundamental wave by generating a sum frequency from the fundamental wave and a seventh harmonic of the fundamental wave. The laser device according to any one of claims 23 to 25, wherein: 27. The wavelength conversion section, comprising: a second nonlinear optical crystal that generates a second harmonic by generating a second harmonic from the fundamental wave; and a sum frequency generation from the fundamental wave and the second harmonic. A third nonlinear optical crystal that generates a third harmonic of the fundamental wave, and a fourth harmonic of the fundamental wave that generates a second harmonic of the second harmonic.
A fourth nonlinear optical crystal for generating a harmonic, and a fifth for generating a seventh harmonic of the fundamental wave by sum frequency generation from a third harmonic of the fundamental wave and a fourth harmonic of the fundamental wave. 27. The laser device according to claim 26, further comprising a nonlinear optical crystal. 28. The first to fourth nonlinear optical crystals are LiB ₃ O ₅ (LBO) crystals, and the fifth nonlinear optical crystal is β-BaB ₂ O ₄ (BBO)
The laser apparatus according to claim 27, characterized in that a crystalline or CsLiB ₆ O ₁₀ (CLBO) crystals. 29. The single-wavelength oscillation laser according to claim 1,
a DFB semiconductor laser or a fiber laser having an oscillation wavelength in the range of μm to 1.59 μm, wherein the wavelength conversion unit generates a wavelength of 151 nm to 159 nm.
24. The laser device according to claim 23, wherein the laser device generates a tenth harmonic that is within the range described above. 30. The single-wavelength oscillating laser has a wavelength of 1.57.
a laser beam having an oscillation wavelength in the range of μm to 1.58 μm; and the wavelength conversion section generates one laser beam in the range of 157 nm to 158 nm whose generation wavelength is substantially the same as the oscillation wavelength of the F ₂ laser.
30. The laser device according to claim 23, wherein the laser device generates a 0th harmonic. 31. The laser light generating section having a wavelength of 1.1.
a single-wavelength laser light near μm, and the wavelength conversion unit generates a fundamental wave near the wavelength of 1.1 μm output from the optical amplifier as a 7th harmonic ultraviolet light. Claims 1 to 22
The laser device according to claim 1. 32. The single wavelength oscillation laser according to claim 1, wherein
a DFB semiconductor laser or a fiber laser having an oscillation wavelength in the range of μm to 1.12 μm, wherein the wavelength conversion unit has a generation wavelength of 147 nm to 160 nm.
32. The laser device according to claim 31, wherein a seventh harmonic within the range is generated. 33. The single-wavelength oscillating laser comprises: 1.09
A laser beam having an oscillation wavelength in the range of 9 μm to 1.106 μm is generated, and the wavelength conversion unit generates a laser beam in the range of 157 nm to 158 nm, which is substantially the same wavelength as the oscillation wavelength of the F ₂ laser.
33. The laser device according to claim 31, wherein the laser device generates a second harmonic. 34. The laser device according to claim 31, wherein the single-wavelength oscillation laser is an ytterbium-doped fiber laser. 35. An exposure apparatus using the laser device according to any one of claims 1 to 34 as a light source. 36. An illumination optical system for irradiating the mask with ultraviolet light emitted from the laser device, and a projection optical system for projecting, on a substrate, a pattern image of the mask irradiated and transmitted or reflected by the ultraviolet light. 36. The exposure apparatus according to claim 35, further comprising: 37. A laser device having a plurality of fiber amplifiers, wherein the output end of the optical amplifier divides a plurality of fiber output ends and has a plurality of output groups formed by bundling. 37. The apparatus according to claim 35, wherein an ultraviolet light output corresponding to at least one of the output groups is used as an alignment light source of the exposure apparatus. Exposure equipment. 38. A projection optical system for projecting a pattern image of a mask onto a substrate, and an ultraviolet light emitted from the laser device is converted into a mark pattern arranged on an object plane or an image plane of the projection optical system. The exposure apparatus according to any one of claims 35 to 37, further comprising a pattern detection system for irradiation. 39. An exposure apparatus for transferring a mask pattern image onto a substrate, comprising: a laser device for emitting a laser beam of a single wavelength; a first fiber optical amplifier for amplifying the laser beam; A light source having a light branching unit for branching the laser light into a plurality of light beams, a second fiber optical amplifier for amplifying the plurality of branch light beams, and a transmission optical system for transmitting the laser light emitted from the light source to an exposure apparatus An exposure apparatus comprising: 40. The laser device according to claim 30, further comprising a wavelength converter that emits infrared light or visible light and that converts laser light emitted from the second fiber optical amplifier into ultraviolet light. An exposure apparatus according to claim 39. 41. The exposure apparatus according to claim 39, wherein the light source has optical means for reducing coherence of the plurality of branched lights. 42. A light source for generating continuous light, an optical modulator for converting the continuous light into pulse light, a first fiber optical amplifier for amplifying the pulse light, and a second fiber amplifier for amplifying the amplified pulse light. A laser device comprising a two-fiber optical amplifier. 43. A fiber optical amplifier further comprising an optical branching means on at least one of the first and second fiber optical amplifiers on the incident side, wherein the pulse light split into a plurality of light beams by the optical branching means is arranged at a subsequent stage. The laser device according to claim 42, wherein the laser beam is incident on the laser beam. 44. The apparatus according to claim 43, further comprising a delay unit for delaying each of the plurality of divided pulse lights and inputting the delayed pulse light to a fiber optical amplifier disposed downstream of the optical branching unit. Laser device. 45. The laser device according to claim 42, wherein the second fiber optical amplifier is a large mode diameter fiber. 46. The first and second fiber optical amplifiers each include a quartz fiber, a silicate-based fiber,
The laser device according to any one of claims 42 to 45, wherein the laser device is any one of a fiber and a fluoride fiber. 47. The continuous light is infrared light or visible light, and further comprises a wavelength converter for converting the wavelength of the pulse light amplified by the second fiber optical amplifier to ultraviolet light. The laser device according to any one of claims 42 to 46. 48. The second fiber optical amplifier is a ZBL
The laser device according to claim 47, wherein the laser device is an AN fiber. 49. The apparatus according to claim 42, further comprising at least one third fiber optical amplifier disposed between the first and second fiber optical amplifiers. A laser device according to claim 1. 50. An illumination optical system, comprising: the laser device according to claim 42; and irradiating the mask with pulse light amplified by the second fiber optical amplifier; An exposure apparatus comprising: an adjustment device that adjusts at least one of oscillation, intensity, and wavelength of pulsed light. 51. The exposure apparatus according to claim 50, wherein the adjustment device has a first controller that controls the oscillation and magnitude of a control pulse applied to the optical modulator. 52. The exposure apparatus according to claim 50, wherein the adjustment device has a second controller that controls a gain of at least one of the first and second fiber optical amplifiers. . 53. The apparatus according to claim 50, wherein the adjusting device has a third controller for controlling the temperature of the light source.
53. The exposure apparatus according to claim 52. 54. An apparatus according to claim 50, further comprising an alignment system for detecting a mark formed on said mask, and a transmission system for guiding at least a part of said amplified pulsed light to said alignment system. 54. The exposure apparatus according to claim 53. 55. The exposure apparatus according to claim 54, wherein the transmission system has first and second fibers for guiding the amplified pulse light to the illumination optical system and the alignment system, respectively. . 56. The apparatus further comprising a plurality of wavelength converters for converting the wavelength of the amplified pulse light into ultraviolet light, wherein a first wavelength converter of the plurality of wavelength converters includes the second fiber optical amplifier and the second fiber optical amplifier. The exposure apparatus according to claim 55, wherein the exposure apparatus is provided between a first fiber and between the first fiber and the illumination optical system. 57. The first wavelength conversion unit is provided between the first fiber and the illumination optical system, and is held integrally with at least a part of the illumination optical system. 59. An exposure apparatus according to item 56. 58. A second wavelength conversion section of the plurality of wavelength conversion sections is provided between the second fiber optical amplifier and the second fiber or between the second fiber and the alignment system. 57. The method according to claim 56, wherein
An exposure apparatus according to claim 57. 59. The apparatus according to claim 58, wherein the second wavelength converter is provided between the second fiber and the alignment system, and is held integrally with at least a part of the alignment system. 3. The exposure apparatus according to claim 1. 60. A projection optical system for projecting at least a part of a pattern formed on the mask on a substrate, and a projection magnification of the projection optical system for scanning and exposing the entire pattern on the substrate. The exposure apparatus according to any one of claims 50 to 59, further comprising a driving device that synchronously moves the mask and the substrate at a substantially corresponding speed ratio. 61. A continuous light emitted from a light source is converted into pulsed light, the pulsed light is amplified a plurality of times by a plurality of fiber optical amplifiers, and the amplified pulsed light is irradiated on a mask. Exposing the substrate with the pulsed light via a substrate. 62. The light source generates a continuous light in an infrared region or a visible region, and converts the wavelength of the pulse light into ultraviolet light before the pulse light is irradiated on the mask. 61. The exposure method according to 61. 63. irradiating at least a part of the ultraviolet light on a mark on the mask prior to exposing the substrate,
63. The exposure method according to claim 62, wherein position information of the mark is detected. 64. The wavelength of the ultraviolet light is controlled by adjusting a temperature of the light source.
3. The exposure method according to 3. 65. The intensity of the ultraviolet light is adjusted by controlling at least one of an optical modulator for converting the continuous light into the pulse light and the plurality of fiber optical amplifiers. The exposure method according to any one of items 62 to 64. 66. The exposure method according to claim 65, wherein the oscillation interval of the ultraviolet light is adjusted by controlling a repetition frequency of the pulse light defined by the light modulator. 67. An oscillation interval of the ultraviolet light, which is disposed between the optical modulator and one of the plurality of fiber optical amplifiers, and controls a time-division optical branching unit that time-divides the pulse light into a plurality. 67. The exposure method according to claim 65, wherein: is adjusted. 68. A device manufacturing method comprising a step of transferring a device pattern onto the substrate by using the exposure method according to claim 61. 69. The light modulator according to claim 42, wherein the light modulator causes the light source to perform pulse oscillation by current control, and reduces a pulse width of pulse light oscillated from the light source by an optical modulation element. The laser device according to claim 44. 70. A control apparatus for controlling at least one of the light source and the optical modulator so as to compensate for an output variation of the pulse light output from the second fiber optical amplifier. Claims 42 to 4
5. The laser device according to claim 4. 71. The exposure apparatus according to claim 50, wherein the adjusting device controls the current of the light source to cause the light source to perform pulse oscillation.