JP2013190517A - Harmonic generator - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a harmonic generator which uses a light source, as a light source of fundamental waves, obtained by optically combining a fiber grating with a solid laser oscillation body and made to be an external resonator, and which suppresses output variation caused by return of return light, when harmonics are highly efficiently emitted.SOLUTION: The harmonic generator includes: a solid laser oscillation body 2; a fiber grating 3 which forms an external resonator 1 with the solid laser oscillation body 2 and emits fundamental waves B; and a wavelength conversion element 9 having a periodical polarization inversion structure 8, for converting a wavelength of the fundamental wave and emitting a harmonic D. The periodical polarization inversion structure 8 includes a chirp period part for suppressing return light.

Description

  The present invention relates to a harmonic generator.

Blue lasers are commercialized with GaN-based semiconductor materials and are already in practical use as light sources for displays. At present, the GaN semiconductor laser is being used to increase the oscillation wavelength, and the laser oscillation is being confirmed to near the green band. However, GaN-based semiconductor lasers, including commercially available blue lasers, have the problem of high power consumption.
On the other hand, a laser using a wavelength conversion element requires a larger number of parts to assemble, but consumes less power and has a better beam quality output from the waveguide. Even if it exists, it has the advantage that the utilization efficiency of light is high. In addition, since the wavelength is stable, the measurement application has a feature that low noise can be measured.

  Examples of the crystal having a non-linear effect used for the wavelength conversion element include lithium niobate and lithium tantalate single crystals. These crystals have high second-order nonlinear optical constants. By forming a periodic domain-inverted structure in these crystals, quasi-phase-matched (QPM) second harmonic generation (Second- Harmonic-Generation (SHG) devices can be realized. In addition, by forming a waveguide in this periodically poled structure, a highly efficient SHG device can be realized, and the wavelength is suitable not only for display applications but also for optical communication, medical use, photochemistry use, various optical measurement uses, etc. Can be designed relatively freely, and can be used in a wide range of applications.

  In wavelength conversion by quasi-phase matching, phase matching conditions can be established in a pseudo manner by nonlinear grating, and high conversion efficiency can be realized in proportion to the square of the length of the wavelength conversion element. However, the width of the wavelength tolerance that satisfies the phase matching condition decreases in inverse proportion to the action length of the grating. For example, in a quasi-phase matching type SHG element using LiNbO3 with a length of 10 mm, the wavelength inversion period is taken as an example in which light with a wavelength of 850 nm is converted to a second harmonic with a wavelength of 425 nm. About 3.2 μm. At this time, the wavelength tolerance of the fundamental wave for satisfying the quasi-phase matching condition is 0.1 nm or less at the full width at half maximum. This value is a very severe value when performing stable wavelength conversion, and there has been a problem that the output becomes unstable due to environmental changes such as ambient temperature.

  In order to solve this problem, Patent Document 1 (Japanese Patent Laid-Open No. 2000-321610) expands the tolerance of the phase matching wavelength by changing the polarization inversion period in a chirp shape. Specifically, the allowable width of the phase matching wavelength can be increased by a linear chirp structure that increases the period of polarization inversion in proportion to the distance.

JP 2000-321610 A

  The inventor has attempted to oscillate harmonics with high efficiency by using a light source that is an external resonator by optically coupling a fiber grating to a solid-state laser oscillator as a fundamental light source. In this case, the wavelength shift of the fundamental wave was precisely controlled by using a fiber grating to reduce the wavelength shift of the fundamental wave as much as possible. At the same time, an attempt was made to achieve high wavelength conversion efficiency by improving the accuracy of the period of the periodically poled structure. By suppressing the wavelength shift of the fundamental wave, even if the manufacturing accuracy of the period is improved and the phase matching wavelength width is reduced, it should have been possible to suppress the reduction in harmonic generation efficiency and instability due to peak out. .

  However, when actually making a prototype, fluctuations in the harmonic oscillation output may occur over time. As a result of the study of the cause by the present inventor, the cause of the output fluctuation was not the fine shift of the phase matching wavelength but the oscillation of the return light having a wavelength slightly different from the fundamental wave wavelength.

  An object of the present invention is to use a light source that is an external resonator by optically coupling a fiber grating to a solid-state laser oscillator as a fundamental wave light source, and when returning harmonics with high efficiency, It is to suppress the output fluctuation caused by the feedback.

The present invention
Solid-state laser oscillator,
This solid-state laser oscillator and an external resonator constitute a fiber grating that oscillates the fundamental wave, and a wavelength conversion element that has a periodic polarization reversal structure that oscillates the harmonic by converting the wavelength of the fundamental wave. The polarization inversion structure includes a chirp period portion that suppresses return light from the periodic polarization inversion structure.

  For example, when the fundamental wave T having a wavelength of 976 nm is made incident on the wavelength conversion element as shown in FIG. I found out that The wavelength of the return light deviates from the phase matching wavelength, and does not cause a peak out of the phase matching wavelength, but is unknown. In order to investigate the cause of the generation of this unknown return light, the present inventor has measured the wavelength characteristics using an element having no periodic structure. As a result, only a wavelength of 976 nm fixed by a fiber grating was observed, and oscillation at 992 nm was not confirmed. In addition, although phase matching was not performed at a wavelength of 976 nm, similar measurement was performed using another wavelength conversion element having a different polarization inversion period, and return light was confirmed at a wavelength different from 992 nm. From these, it was considered that the cause of the return light was due to the periodic structure of polarization inversion of the wavelength conversion element.

  As a result of various studies to reduce the output fluctuation due to the return light, the present inventor has significantly reduced the return light as shown in FIG. 7, for example, by providing a chirp period portion in the periodically poled structure. The inventors have found that fluctuations are suppressed and have reached the present invention.

It is a schematic diagram which shows a harmonic generator. It is a chart which shows fundamental wave T and return light N in one embodiment. It is a schematic diagram which shows an example with a constant period in a periodic polarization inversion structure. It is a schematic diagram which shows the example whose period is a chirp periodic structure in a periodic polarization inversion structure. It is a schematic diagram which shows the example whose period is a chirp periodic structure in a periodic polarization inversion structure. It is a schematic diagram which shows the example whose period is a chirp periodic structure in a periodic polarization inversion structure. It is a chart which shows the example in which return light N was controlled.

  FIG. 1 is a block diagram schematically showing a harmonic generator according to an embodiment of the present invention. The light source 1 includes a solid-state laser oscillation source 2 and a fiber grating 3. Laser light A is oscillated from the solid-state laser light source 2. The laser beam A enters the fiber 4, is guided, and enters the fiber grating 3. Here, the laser beam is subjected to wavelength selection, and a fundamental wave having extremely high coherency is emitted. The fundamental wave B is collected by the optical system 5 and is incident on one end face 10 a of the wavelength conversion unit 10 of the wavelength conversion element 9.

  In this example, the wavelength conversion element 9 is made of a ferroelectric substrate, and a periodically poled structure 8 is formed in the substrate. In this example, the periodic polarization inversion structure 8 is formed from one end face 10a of the conversion unit 10 of the wavelength conversion element 9 to the other end face 10b. The fundamental wave B incident on the end face 10 a generates a harmonic while propagating through the conversion unit 10. And the fundamental wave C and the harmonic wave D are radiate | emitted outside from the output surface 10b.

  Here, as shown in FIG. 3, the periodically poled structure 8 has a large number of alternately domain-inverted portions 8a and non-inverted portions 8b. Here, the sum of the width of the polarization inversion portion 8a and the width of the non-inversion portion 8b is the period P. Here, the present inventor has attempted to make the period P as close as possible to the constant value PO in order to increase the oscillation efficiency. However, it has been found that when the manufacturing accuracy is improved, the return light N is generated at a position slightly apart from the fundamental wave T as shown in FIG.

  Therefore, for example, as shown in FIG. 4, the period P was smoothly changed to obtain a chirp periodic structure. As a result, for example, as shown in FIG. 7, it was found that unnecessary return light N is suppressed and output fluctuations of harmonics are suppressed.

  Here, the chirp periodic structure has the effect of suppressing the return light N, but since the wavelength shift of the fundamental wave is small, it does not suppress the output decrease due to the peak-out of the phase matching wavelength.

  As the solid-state laser oscillator, a laser with a highly reliable GaAs-based or InP-based material is suitable. For example, in the case of a green laser, a GaAs laser that oscillates near a wavelength of 1064 nm is used. Since GaAs-based and InP-based lasers have high reliability, a light source such as a one-dimensionally arranged laser array can be realized.

  A fiber grating is one in which a periodic refractive index change is formed in the core of an optical fiber. The fiber grating used in the present invention functions as a reflection filter that selectively reflects only light of that wavelength in order to stabilize the excitation wavelength of the solid-state laser oscillator.

The fiber grating can be adjusted, for example, by increasing the reflectivity or expanding the reflected wavelength band, depending on the design of the grating. If the reflectance is increased, the influence of reflection from the outside can be reduced, and the wavelength of the solid-state laser oscillator can be stabilized. However, the higher the reflectivity, the lower the output of extraction. As a result, a large wavelength converted light cannot be obtained. Therefore, the reflectance of the grating cannot be increased so much that large wavelength converted light can be obtained.

  In the present invention, a chirp period portion is provided in the periodically poled structure. The chirp period portion means a portion in which the inversion period P changes within a predetermined range in the periodically poled structure.

  In a preferred embodiment, the chirp period portion has a monotone increasing portion where the cycle increases monotonously and a monotone decreasing portion where the cycle decreases continuously, and both are alternately arranged. This structure is particularly effective in suppressing the above-described return light, and can also increase the oscillation intensity of harmonics.

  For example, in the element of FIG. 4, the inversion period P includes alternating monotonously increasing portions LU and monotonously decreasing portions LD. In this example, in the monotonically increasing portion LU, the period P increases linearly with respect to the position x in the length direction, and in the monotonous decreasing portion LD, the period P increases linearly with respect to the position x in the length direction. It is decreasing functionally. As a result, the period P moves up and down between the maximum value PU and the minimum value PD.

  In the example of FIG. 5, the inversion period P includes alternating monotonously increasing portions LU and monotonically decreasing portions LD. In this example, in the monotonically increasing portion LU, the period P increases sinusoidally with respect to the position x in the length direction, and in the monotonous decreasing portion LD, the period P increases in sine with respect to the position x in the length direction. It is decreasing functionally. As a result, the period P moves up and down between the maximum value PU and the minimum value PD.

  In the example of FIG. 6, the period P monotonously increases from the minimum value PD toward the maximum value PU. The period P may monotonously decrease from the incident side toward the emission side.

  When the period P monotonously increases or monotonously decreases, it may increase or decrease in a linear function or increase or decrease in a sine function with respect to the position x in the length direction of the element. However, this function is not limited. For example, the period P may increase or decrease in a quadratic function or a cubic function with respect to the position x, or may increase or decrease in an arc shape. Furthermore, the period P may increase or decrease discretely with respect to x, but from the viewpoint of improving the oscillation efficiency of the harmonics, the period P should increase and decrease monotonously. Is preferred.

  When the average value of the period P is PO, the maximum value is PU, and the minimum value is PD, (PU-PD) / PO is preferably 0.002 or more from the viewpoint of suppressing the return light, 0.005 The above is more preferable. Further, (PU-PD) / PO is preferably 0.05 or less, and more preferably 0.02 or less, from the viewpoint of increasing the oscillation intensity of the harmonic.

  The average period PO is not limited because it is determined by the target phase matching wavelength and the refractive index of the material, but when phase matching is performed at a wavelength of 810 nm, the average period PO is 2.7-2. The average value PO of the phase matching at the wavelength of 1064 nm is preferably 6.5 to 6.7 μm. When the phase matching is performed at the wavelength of 1550 nm, the average value PO of the cycle is 17. It is preferably 4 to 17.8 um. The relationship between the phase matching wavelength and the average period value PO has a substantially linear relationship.

  The periodically poled structure may be formed over the entire length of the element or may be formed only on a part of the element. Further, the chirp period portion may occupy the entire length of the periodically poled structure, but may occupy only a part. When the chirp period portion occupies a part of the periodically poled structure, it is preferable that the remaining period is constant.

  The difference between the wavelength of the fundamental wave T and the wavelength of the return light N is usually 5 nm or more, preferably 10 nm or more. Further, this difference is usually 50 nm or less, preferably 30 nm or less, and further 25 nm or less. Although depending on the structure of the waveguide, the wavelength of the return light N is often on the long wavelength side with respect to the wavelength of the fundamental wave T, but may be generated on the short wavelength side due to manufacturing factors. .

  In a preferred embodiment, the periodically poled structure 8 is provided in the channel type optical waveguide 10 in the element 9. In a particularly preferred embodiment, the optical waveguide is a ridge-type optical waveguide, and is obtained by physically processing and shaping a nonlinear optical crystal, for example, by machining or laser processing.

  The material constituting the wavelength conversion element is not particularly limited as long as it can modulate light, but lithium niobate, lithium tantalate, lithium niobate-lithium tantalate solid solution, potassium lithium niobate, KTP, GaAs, crystal, etc. Can be illustrated.

  In the ferroelectric single crystal, at least one selected from the group consisting of magnesium (Mg), zinc (Zn), scandium (Sc), and indium (In) in order to further improve the optical damage resistance of the optical waveguide. The metal element can be contained, and magnesium is particularly preferable. The ferroelectric single crystal can contain a rare earth element as a doping component. This rare earth element acts as an additive element for laser oscillation. As this rare earth element, Nd, Er, Tm, Ho, Dy, and Pr are particularly preferable.

  In a preferred embodiment, the wavelength conversion element is bonded to a separate support substrate. The specific material of the support substrate is not particularly limited, and examples thereof include glass such as lithium niobate, lithium tantalate, and quartz glass, quartz, and Si. The material of the adhesive layer (not shown) may be an inorganic adhesive, an organic adhesive, or a combination of an inorganic adhesive and an organic adhesive.

(Comparative example)
The oscillation device described with reference to FIGS. 1 and 3 was produced.
Specifically, a comb-like periodic electrode was formed on a 0.5 mm-thick MgO 5% doped lithium niobate 5 degree off-cut Y substrate 9 by photolithography. After forming the electrode film over the entire surface of the substrate, a periodic voltage inversion structure 8 was formed by applying a pulse voltage.

  After forming a periodically poled structure on the substrate, a SiO 2 under clad having a thickness of 0.4 μm was formed by sputtering. After an adhesive was applied to a non-doped lithium niobate substrate having a thickness of 0.5 mm, it was bonded to the MgO-doped lithium niobate substrate, and the surface of the MgO-doped lithium niobate substrate was ground and polished to a thickness of 3.5 μm. . Then, the ridge type waveguide 10 was formed by a laser ablation processing method. The digging amount at both ends of the ridge waveguide grooved by laser ablation was 2.3 μm, and the width of the upper part of the ridge was 5.2 μm.

  However, the period P was set to a constant period PO = 0.08 μm in the element having a length of 8 mm. After the optical waveguide was formed, it was cut with a dicer to a length of about 12 mm and a width of 0.7 mm, and this element was set on a surface plate and a jig, and both end surfaces were polished to form a polished surface. Next, an antireflection film was formed on the end face.

  The solid laser oscillator 2 and the fiber grating 3 were as follows. As the solid-state laser resonator 2, a GaAs semiconductor laser that oscillates in the vicinity of a wavelength of 980 nm is used. As the fiber grating 3, one having a reflection wavelength of 976 nm and a reflectance of 3% was used.

  Each component and the wavelength conversion element shown in FIG. 1 were adjusted in optical axis, fixed with resin, and then mounted in the apparatus.

  The fiber grating 3 is controlled so that the fundamental wave having a wavelength of 976 nm is stably oscillated from the light source 1, and light having an output of about 80 mW is incident on the wavelength conversion element. Oscillated. This output was 11 mW at maximum, but it fluctuated greatly with time and was not stable.

(Example)
An oscillation device was fabricated in the same manner as in the comparative example.
However, in the element having a length of 12 mm, the period P was increased and decreased at intervals of 2 mm in a triangular wave shape as shown in FIG. 4 between the minimum period PD = 5.06 um and the maximum period PU = 5.10 um. The average PO of the polarization inversion period is 5.08 um.

  As in the comparative example, light having an output of about 80 mW was made incident on the wavelength conversion element. This output was about 8 mW on average. Although the maximum output decreased slightly compared with the comparative example, the output was stable. Moreover, in the design of this wavelength conversion element, reflection from the element was suppressed, and oscillations of wavelengths other than the excitation light were not observed.

Claims (2)

Solid-state laser oscillator,
This solid-state laser oscillator and an external resonator constitute a fiber grating that oscillates a fundamental wave, and a wavelength conversion element that has a periodic polarization inversion structure that oscillates a harmonic by converting the wavelength of the fundamental wave, The harmonic generation device, wherein the periodically poled structure includes a chirp period portion that suppresses return light.   The chirp period part includes a monotonically increasing part in which the polarization inversion period monotonously increases, and a monotonically decreasing part in which the polarization inversion period monotonously decreases, and the monotonically increasing part and the monotonously decreasing part are provided alternately. The device according to claim 1, wherein:

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