JP5749553B2 - Light modulation control method, control program, control device, and laser light irradiation device - Google Patents

Description

  The present invention relates to a light modulation control method, a control program, a control device, and a laser beam using the same, which control condensing irradiation of laser light to a condensing point by a modulation pattern presented to a plurality of pixels of a spatial light modulator The present invention relates to an irradiation apparatus.

  In recent years, active research has been conducted on three-dimensional fabrication of optical integrated circuits such as waveguides, optical splitters, and directional couplers inside glass. One method for manufacturing such an optical integrated circuit is a method using femtosecond laser light. In this method, for example, an impact is induced by two-photon absorption or the like at the condensing point of the femtosecond laser beam, and thereby processing for locally changing the refractive index of the glass can be performed. In addition to the fabrication of optical integrated circuits, such focused irradiation of laser light onto an object to be irradiated is widely used in various laser processing apparatuses or laser microscopes that observe scattering and reflection of laser light. (For example, refer to Patent Documents 1 to 3 and Non-Patent Documents 1 to 6).

  Here, when laser light irradiation such as processing of a complicated three-dimensional structure is performed using one laser light beam emitted from a laser light source, there is a problem that an enormous time is required for the processing step. As a method for shortening the processing time in this case, a method of performing multi-point simultaneous processing using a plurality of condensing points is conceivable. The simplest configuration for realizing such a method is a configuration using a plurality of laser light beams supplied from a plurality of laser light sources. However, such a configuration is not realistic in view of the cost of preparing a plurality of laser light sources, installation space, and the like.

  On the other hand, a method of realizing multi-point simultaneous processing using a phase modulation type spatial light modulator (SLM) and a hologram (CGH: Computer Generated Hologram) obtained by numerical calculation has been studied. Yes. When laser light is input to the spatial light modulator on which CGH is presented, the phase of the input light is modulated according to the modulation pattern of CGH. When the wave front of the modulated laser light output from the optical modulator is condensed by a Fourier transform lens, a plurality of condensing points can be created from one laser light beam, and simultaneous processing by multi-point simultaneous irradiation Laser operation such as simultaneous observation becomes possible.

  In multi-point simultaneous processing inside an irradiation object (processing object) using a spatial light modulator, laser light can be condensed at an arbitrary position in one plane perpendicular to the optical axis. In such multi-point simultaneous processing, by using a method such as presenting a Fresnel lens pattern having a lens effect on a spatial light modulator, laser light can be applied to an arbitrary three-dimensional position including the optical axis direction. It is also possible to collect light.

JP 2010-058128 A JP 2010-075997 A Japanese Patent No. 4300101

J. Bengtsson, "Kinoformdesign with an optimal-rotation-angle method", Appl. Opt. Vol.33 No.29 (1994) pp.6879-6884 J. Bengtsson, "Design of fan-out kinoforms in the entire scalar diffraction regime with anoptimal-rotation-angle method", Appl. Opt. Vol. 36 No. 32 (1997) pp. 8435-8444 N. Yoshikawa et al., "Phaseoptimization of a kinoform by simulated annealing", Appl. Opt. Vol.33 No.5 (1994) pp.863-868 N. Yoshikawa et al., "Quantized phase optimization of two-dimensional Fourier kinoforms by a genetic algorithm", Opt. Lett. Vol.20 No.7 (1995) pp.752-754 C. Mauclair et al., "Ultrafastlaser writing of homogeneous longitudinal waveguides in glasses using dynamicwavefront correction", Opt. Exp. Vol.16 No.8 (2008) pp.5481-5492 A. Jesacher et al., "Paralleldirect laser writing in three dimensions with spatially dependent aberration correctionion", Opt. Exp. Vol.18 No.20 (2010) pp.21090-21099 Hiroshi Kubota, "Optics", Iwanami Shoten, 1967, pp. 128-131, pp. 300-301 Y. Ogura et al., "Wavelength-multiplexing diffractive phaseelements: design, fabrication, and performance evaluation", J. Opt. Soc. Am.A Vol.18 No.5 (2001) pp.1082-1092

  In the above-mentioned focused irradiation of laser light onto the irradiation target, if there is an aberration object on the propagation path of the laser light from the spatial light modulator to the irradiation target, the propagating laser light is affected by the aberration. become. For example, when processing the inside of the glass by laser light irradiation, in the convergent light emitted from the objective lens, due to the difference in refractive index between the air that is the atmosphere medium and the glass medium that is the processing target, Misalignment (aberration) occurs.

  When such aberration occurs, the shape of the condensing point of the laser light extends in the optical axis direction, and the condensing density at the condensing point decreases. In this case, when processing the object, the incident laser light intensity must be increased in order to make the laser light intensity at the condensing point reach the processing threshold, or fine processing is performed because the condensing shape is extended. Problems such as being unable to do so occur. Such a problem of the influence of aberration occurs not only in the case of multi-point simultaneous irradiation but also in the case of condensing and irradiating a single condensing point with laser light.

  The present invention has been made to solve the above-described problems, and an optical modulation control method, an optical modulation control program, and an optical modulation capable of suitably controlling the condensing state of laser light at the condensing point. It aims at providing a control apparatus and a laser beam irradiation apparatus using the same.

In order to achieve such an object, an optical modulation control method according to the present invention includes (1) a phase modulation type of inputting laser light, modulating the phase of the laser light, and outputting the laser light after phase modulation. A light modulation control method that uses a spatial light modulator to control condensing irradiation of laser light to a set condensing point according to a modulation pattern presented to the spatial light modulator, and (2) irradiation of laser light As conditions, the incident pattern of the laser light to the spatial light modulator, the first refractive index n ₁ of the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point, and the first propagation medium An irradiation condition acquisition step of acquiring a second refractive index n ₂ different from the first refractive index of the second propagation medium closer to the condensing point side, and (3) a spatial light modulator as the laser light condensing condition the number s _{t (s t} of the focal point of the laser beam focused irradiation from two or more Integer), and s _t number of condensing positions of the respective focal point s, and the condensing condition setting step of setting the current intensity, (4) the laser light from the spatial light modulator to the focusing point s In consideration of the aberration condition derived in the aberration condition deriving step, and (5) the aberration condition deriving step for deriving the aberration condition caused by the first propagation medium and the second propagation medium having different refractive indexes, A modulation pattern design step for designing a modulation pattern to be presented to the spatial light modulator, and (6) the modulation pattern design step assumes a plurality of pixels arranged two-dimensionally in the spatial light modulator, Focusing on the effect of changing the phase value at one pixel of the modulation pattern to be presented on the condensing state of the laser beam at the condensing point, changing the phase value so that the condensing state approaches a desired state, That Such a phase value change operation is performed on all the pixels of the modulation pattern to design the modulation pattern, and when evaluating the condensing state at the condensing point, it collects from the pixel j in the modulation pattern of the spatial light modulator. For propagation of light to the light spot s, a propagation function φ _js ′ obtained by adding an aberration condition to the wave propagation function φ _js of free propagation in a state where the propagation medium is homogeneous is used , and the aberration condition derivation step is performed from the pixel j. As an aberration condition for the propagation of light to the condensing point s, a phase Φ _j-OPD that gives an optical path length difference in the propagation is obtained, and the modulation pattern design step is performed by a conversion equation.
φ _js ' = φ _js + Φ _j-OPD
Accordingly, characterized Rukoto seek propagation function phi _js' aberration condition is considered.

An optical modulation control program according to the present invention uses (1) a phase modulation type spatial light modulator that inputs laser light, modulates the phase of the laser light, and outputs the laser light after phase modulation. A program for causing a computer to execute light modulation control for controlling the condensing irradiation of laser light to a set condensing point according to a modulation pattern presented to the optical modulator, and (2) laser light irradiation conditions From the incident pattern of the laser light to the spatial light modulator, the first refractive index n ₁ of the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point, and the first propagation medium Also, an irradiation condition acquisition process for acquiring a second refractive index n ₂ different from the first refractive index of the second propagation medium on the condensing point side, and (3) from the spatial light modulator as the laser light condensing condition Number of focusing points s _{t for} focusing and irradiating the laser beam (S _t is an integer of 2 or more), and a condensing condition setting process for setting a condensing position and a condensing intensity for each of the s _t condensing points s, and (4) condensing from the spatial light modulator An aberration condition deriving process for deriving an aberration condition caused by the first propagation medium and the second propagation medium having different refractive indexes in the propagation of the laser beam to the point s, and (5) the aberration derived by the aberration condition deriving process. In consideration of the conditions, the computer executes a modulation pattern design process for designing a modulation pattern to be presented to the spatial light modulator. (6) The modulation pattern design process includes a plurality of two-dimensionally arranged modulation patterns in the spatial light modulator. Assuming a pixel, paying attention to the effect of changing the phase value in one pixel of the modulation pattern presented to a plurality of pixels on the condensing state of the laser beam at the condensing point, the condensing state becomes a desired state Set the phase value closer In addition, the modulation pattern is designed by performing such a phase value changing operation for all the pixels of the modulation pattern, and the modulation pattern of the spatial light modulator is evaluated when evaluating the light collection state at the light collection point. for propagation of light from the pixel j to the focal point s, the propagation medium is converted by adding aberration condition the wave propagation function phi _js the free propagation of the homogeneous state transfer function phi _js' used in aberration condition deriving process Obtains a phase Φ _j-OPD that gives an optical path length difference in the propagation as an aberration condition for the propagation of light from the pixel j to the condensing point s.
φ _js ' = φ _js + Φ _j-OPD
Accordingly, characterized Rukoto seek propagation function phi _js' aberration condition is considered.

The light modulation control apparatus according to the present invention uses (1) a phase modulation type spatial light modulator that inputs laser light, modulates the phase of the laser light, and outputs the laser light after phase modulation. An optical modulation control device for controlling the condensing irradiation of laser light to a set condensing point according to a modulation pattern presented to the optical modulator, and (2) as a laser light irradiation condition, to the spatial light modulator The incident pattern of the laser light, the first refractive index n _{1 of} the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point, and the condensing point side of the first propagation medium An irradiation condition acquiring means for acquiring a second refractive index n ₂ different from the first refractive index of the second propagation medium; and (3) condensing and irradiating the laser light from the spatial light modulator as the condensing condition of the laser light. Number of focusing points s _t (s _t is an integer of 2 or more), and s _t focusing points a condensing condition setting means for setting a condensing position and a condensing intensity for each of s, and (4) a first propagation having a different refractive index in the propagation of laser light from the spatial light modulator to the condensing point s. An aberration condition deriving unit for deriving an aberration condition caused by the medium and the second propagation medium, and (5) designing a modulation pattern to be presented to the spatial light modulator in consideration of the aberration condition derived by the aberration condition deriving unit (6) The modulation pattern design means assumes a plurality of pixels arranged two-dimensionally in the spatial light modulator, and calculates a phase value of one modulation pattern to be presented to the plurality of pixels. Paying attention to the effect of the change on the condensing state of the laser beam at the condensing point, the phase value is changed so that the condensing state approaches the desired state, and such an operation of changing the phase value is performed on the modulation pattern. All pixels When designing the modulation pattern and evaluating the light condensing state at the condensing point, the propagation medium is used to propagate light from the pixel j to the condensing point s in the modulation pattern of the spatial light modulator. Using the propagation function φ _js ′ converted by adding the aberration condition to the wave propagation function φ _js in the free propagation in the homogeneous state , the aberration condition deriving means uses the aberration for the light propagation from the pixel j to the condensing point s. As a condition, the phase Φ _j-OPD that gives the optical path length difference in the propagation is obtained, and the modulation pattern design means uses the conversion formula
φ _js ' = φ _js + Φ _j-OPD
Accordingly, characterized Rukoto seek propagation function phi _js' aberration condition is considered.

  In the light modulation control method, the control program, and the control device described above, with regard to the focused irradiation of the laser beam to the focusing point using the spatial light modulator, the incident pattern of the laser beam and the first on the propagation path, Information on the second propagation medium is acquired, and the number of condensing points of the laser light, the condensing position at each condensing point, and the condensing condition including the condensing intensity are set. Then, an aberration condition generated when the first and second propagation media having different refractive indexes are on the propagation path is derived, and a modulation pattern to be presented to the spatial light modulator is designed in consideration of the aberration condition. Thereby, the influence of the aberration by the 1st, 2nd propagation medium can be reduced in the condensing state of the laser beam in each condensing point with respect to the set single condensing point or a plurality of condensing points.

Furthermore, regarding the design of the modulation pattern in such a configuration, specifically, a pixel structure including a plurality of pixels arranged two-dimensionally in the spatial light modulator is assumed. Then, a design method that focuses on the influence of the change of the phase value at one pixel of the modulation pattern on the condensing state of the laser beam at the condensing point is used, and free propagation is performed in the evaluation of the condensing state at the condensing point. rather than using wave propagation function phi _js assuming a, is evaluating condensed state after having converted the propagation function phi _js' aberration condition is considered. According to such a configuration, it is possible to appropriately and reliably evaluate and control the condensing state of the laser light at the condensing point. When a spatial light modulator having a plurality of pixels arranged two-dimensionally is used as the spatial light modulator, the pixel structure can be applied to the design of the modulation pattern as it is.

Here, the light modulation control method, the control program, and the control device described above calculate the optical path length difference in the propagation as the aberration condition for the light propagation from the pixel j to the condensing point s in the derivation of the aberration condition. The phase Φ _j-OPD to be given is obtained, and in the modulation pattern design, the conversion formula φ _js ′ = φ _js + Φ _j-OPD
Thus, it is preferable to obtain the propagation function φ _js ′ in consideration of the aberration condition. According to such a configuration, the propagation function φ _js of free propagation can be suitably converted into a propagation function φ _js ′ in which the aberration condition is considered.

Further, the light modulation control method, the control program, and the control device, in designing the modulation pattern, set the incident amplitude of the laser light to the pixel j of the spatial light modulator as A _j-in , the phase as φ _j-in , and the pixel j. as the phase values phi _j in the following formula _{U s = a s exp (iφ} s)
= Σ _j A _j-in exp (iφ _js ') exp (i (φ _j + φ _j-in ))
Thus, it is preferable to obtain the complex amplitude U _s indicating the condensing state at the condensing point s. Thereby, the condensing state of the laser beam in a condensing point can be evaluated suitably.

As for the specific configuration of the modulation pattern design, in the change of the phase value at the pixel j of the modulation pattern, the propagation function considering the phase φ _{s of the} complex amplitude indicating the condensing state at the condensing point _s and the aberration condition A configuration in which the phase value is changed based on φ _js ′ and a value analytically obtained based on the phase value φ _j before the change at the pixel j can be used. As a method of updating the phase value analytically in this way, for example, there is an ORA (Optimal Rotation Angle) method. Alternatively, in the change of the phase value at the pixel j of the modulation pattern, a configuration in which the phase value is changed by a value obtained by searching using any one of the hill-climbing method, the annealing method, and the genetic algorithm is used. Also good.

  For the first and second propagation media on the propagation path of the laser beam, for example, the second propagation medium is an irradiation object with a condensing point set inside, and the first propagation medium is a space. A configuration that is an atmospheric medium between the light modulator and the irradiation object can be used. The atmosphere medium may be water, oil, or the like in addition to air. There may be three or more media between the spatial light modulator and the condensing point.

  The light modulation control device may include light modulator drive control means for driving and controlling the spatial light modulator and presenting the modulation pattern designed by the modulation pattern design means to the spatial light modulator. Further, such an optical modulator drive control means may be provided as a separate device from the optical modulation control device for designing the modulation pattern.

  The laser light irradiation apparatus according to the present invention includes (a) a laser light source that supplies laser light, and (b) a phase that inputs the laser light, modulates the phase of the laser light, and outputs the modulated laser light after phase modulation. A modulation-type spatial light modulator; and (c) a light modulation control device having the above-described configuration that controls the focused irradiation of the modulated laser beam to the set focal point by the modulation pattern presented to the spatial light modulator. It is characterized by providing.

  According to such a configuration, the light modulation control device suitably and surely controls the condensing state of the laser light at the condensing point, and the laser for a single condensing point or a plurality of condensing points set in the irradiation object. It is possible to suitably realize operations such as focused irradiation of light and processing and observation of an object by the light. Such a laser beam irradiation apparatus can be used as a laser processing apparatus, a laser microscope, etc., for example. As the spatial light modulator, it is preferable to use a spatial light modulator that has a plurality of pixels arranged two-dimensionally and modulates the phase of laser light in each of the plurality of pixels.

  According to the light modulation control method, the control program, the control apparatus, and the laser beam irradiation apparatus using the same according to the present invention, the laser beam is focused on the focused spot using the spatial light modulator. Obtain the incident pattern and the refractive index of the first and second propagation media on the propagation path, set the number of condensing points of the laser light, the condensing position and condensing intensity at each condensing point, 1. Deriving the aberration condition caused by the second propagation medium, and designing the modulation pattern to be presented to the spatial light modulator in consideration of the aberration condition, and in the modulation pattern design, the phase of the modulation pattern in one pixel Using a design method that focuses on the effect of changing the value on the focusing state of the laser beam at the focusing point, and using a propagation function that takes aberration conditions into account when evaluating the focusing state at the focusing point By focusing the laser beam at the condensing point It is possible to suitably and reliably controlled.

It is a figure which shows the structure of one Embodiment of a laser beam irradiation apparatus. It is a figure shown about generation | occurrence | production of the aberration in the propagation process of a laser beam. It is a block diagram which shows an example of a structure of a light modulation control apparatus. It is a flowchart which shows an example of the light modulation control method. It is a figure shown about derivation | leading-out of the aberration conditions produced in the propagation of a laser beam. It is a flowchart which shows an example of the design method of a modulation pattern. It is a figure which shows the example of the irradiation pattern of the laser beam by a laser beam irradiation apparatus. It is a figure which shows the example of the irradiation pattern of the laser beam by a laser beam irradiation apparatus. It is a figure which shows the example of the irradiation pattern of the laser beam by a laser beam irradiation apparatus. It is a flowchart which shows the other example of the design method of a modulation pattern. It is a figure which shows the structure of other embodiment of a laser beam irradiation apparatus. It is a figure shown about an example of the condensing irradiation of the laser beam to an irradiation target object.

  Hereinafter, preferred embodiments of a light modulation control method, a control program, a control apparatus, and a laser light irradiation apparatus according to the present invention will be described in detail with reference to the drawings. In the description of the drawings, the same elements are denoted by the same reference numerals, and redundant description is omitted. Further, the dimensional ratios in the drawings do not necessarily match those described.

  First, a basic configuration of a laser beam irradiation apparatus including a spatial light modulator, which is an object of light modulation control according to the present invention, will be described together with a configuration example thereof. FIG. 1 is a diagram showing a configuration of an embodiment of a laser beam irradiation apparatus including a light modulation control apparatus according to the present invention. The laser beam irradiation apparatus 1 </ b> A according to the present embodiment is a device that condenses and irradiates an irradiation object 15 with laser light, and includes a laser light source 10, a spatial light modulator 20, and a movable stage 18. .

  In the configuration shown in FIG. 1, the irradiation object 15 is placed on a movable stage 18 configured to be movable in the X direction, the Y direction (horizontal direction), and the Z direction (vertical direction). Further, in the present apparatus 1A, a condensing point for processing, observing, etc. of the object 15 is set inside the irradiation object 15, and the condensing irradiation of the laser beam is performed on the condensing point. Is done.

  The laser light source 10 supplies laser light such as pulsed laser light for condensing and irradiating the irradiation target 15 on the stage 18. The laser light output from the laser light source 10 is spread by the beam expander 11 and then input to the spatial light modulator (SLM) 20 via the reflection mirrors 12 and 13.

  The spatial light modulator 20 is a phase modulation type spatial light modulator, and modulates the phase of the laser light at each part of the two-dimensional modulation surface, for example, and outputs the laser light after phase modulation. As the spatial light modulator 20, preferably, a spatial light modulator that has a plurality of pixels arranged two-dimensionally and modulates the phase of laser light in each of the plurality of pixels is used. In such a configuration, the spatial light modulator 20 is presented with a modulation pattern such as CGH, for example, and condensing irradiation of the laser beam to the set condensing point is controlled by this modulation pattern. The spatial light modulator 20 is driven and controlled by the light modulation control device 30 via the light modulator driving device 28. A specific configuration and the like of the light modulation control device 30 will be described later. Further, the spatial light modulator 20 may be one that does not have the pixel structure described above.

  The spatial light modulator 20 may be a reflection type or a transmission type. In FIG. 1, a reflection type is shown as the spatial light modulator 20. Further, as the spatial light modulator 20, a refractive index changing material type SLM (for example, a liquid crystal on silicon (LCOS) type, a liquid crystal display (LCD) type using a liquid crystal), a segment mirror type SLM, or a continuous deformable mirror type is used. SLM, DOE (Diffractive Optical Element), etc. are mentioned. Note that the DOE includes a discrete representation of a phase or a pattern designed using a method described later and converted into a continuous pattern by smoothing or the like.

  The laser light that is phase-modulated into a predetermined pattern by the spatial light modulator 20 and is output is propagated to the objective lens 25 by the 4f optical system including the lenses 21 and 22. Then, the objective lens 25 condenses and irradiates laser light onto one or a plurality of condensing points set on the surface or inside of the irradiation object 15.

  Note that the configuration of the optical system in the laser light irradiation apparatus 1A is not limited to the configuration shown in FIG. 1, and various configurations can be used. For example, in FIG. 1, the laser beam is expanded by the beam expander 11, but a configuration using a combination of a spatial filter and a collimating lens may be used. Further, the drive device 28 may be configured to be integrated with the spatial light modulator 20. For the 4f optical system using the lenses 21 and 22, it is generally preferable to use a double-sided telecentric optical system composed of a plurality of lenses.

  The movable stage 18 for moving the irradiation object 15 may be configured, for example, such that the stage is fixed and a movable mechanism, a galvano mirror, or the like is provided on the optical system side. Further, as the laser light source 10, it is preferable to use a pulse laser light source that supplies pulse laser light, such as an Nd: YAG laser light source or a femtosecond laser light source.

In the laser light irradiation apparatus 1A shown in FIG. 1, when there is an aberration object on the propagation path of the laser light from the spatial light modulator 20 to the condensing point in the irradiation object 15, the laser light has an aberration in the propagation process. to be influenced. Here, FIG. 2 is a diagram illustrating the occurrence of aberration in the propagation process of laser light. For example, when a condensing point is set inside the irradiation object 15 as described above, the convergent laser light output from the objective lens 25 is an atmospheric medium on the propagation path from the objective lens 25 to the condensing point. the refractive index n ₁ of the air is (first propagation medium), the difference between the refractive index n ₂ of the irradiated object (second propagation medium) 15 such as a glass medium, and the paraxial ray, a ray of outermost Thus, the refraction angle at the boundary surface between the atmospheric medium and the irradiation object 15 such as a glass medium is different, and thereby defocus (spherical aberration) occurs.

For example, as shown in FIG. 2, consider a case where the focal point O by the objective lens 25 is at a position of a depth d inside the irradiation target 15. In this case, the focal point O is shifted to the focal point O ′ by the defocus amount δ due to the refraction angle at the boundary surface between the air having the refractive index n ₁ and the object 15 having the refractive index n ₂ . Further, the defocus amount δ varies depending on the incident height h of light incident on the objective lens 25. Due to the spherical aberration due to the defocus δ depending on the incident height h, the shape of the condensing point of the laser beam in the object 15 extends in the optical axis direction, and the condensing density decreases.

  In addition, the generation of aberration due to such a propagation medium is a case where a plurality of condensing points are set inside the irradiation target 15 and multipoint simultaneous irradiation (for example, multipoint simultaneous processing) is performed on the target 15. It also becomes a problem. That is, the spherical aberration described above has a different amount of aberration depending on the condensing position (optical axis depth) of the laser beam in the optical axis direction, and the spherical aberration amount tends to increase as the optical axis depth increases. In this case, when performing three-dimensional multi-point simultaneous irradiation on the object 15, it is necessary to correct a spherical aberration amount that differs depending on the optical axis depth of each condensing position for each condensing point. .

  Moreover, when performing multipoint simultaneous irradiation, there also exists a problem of adjustment of the condensing intensity | strength of the laser beam with respect to each condensing point. For example, in glass internal processing using femtosecond laser light, it is known that the amount of change in the refractive index generated by processing at the target site varies depending on the intensity of the laser light at the focal point. Therefore, when producing multiple waveguides with the same refractive index distribution at the same time by simultaneous multi-point irradiation of laser light, the intensity of light collected at multiple light collection points is determined by the modulation pattern presented on the spatial light modulator. Is preferably reproduced with high uniformity. Conversely, it is also possible to produce a plurality of waveguides having different refractive index distributions by setting the condensing intensities at a plurality of condensing points to different intensities. In any of these cases, when a plurality of condensing points are set, it is desirable that the condensing intensity of the laser light at each condensing point can be arbitrarily controlled.

  On the other hand, the laser light irradiation apparatus 1A in FIG. 1 appropriately designs the CGH of the modulation pattern to be presented to the spatial light modulator 20 via the drive device 28 in the light modulation control device 30 so that the propagation path By reducing the influence of aberration caused by propagation media having different refractive indexes on the upper side, the condensing state of the laser beam at the condensing point is suitably controlled. Further, according to the laser light irradiation apparatus 1A and the light modulation control apparatus 30 according to the present embodiment, when a plurality of condensing points are set, three-dimensional multi-point laser light irradiation and between the condensing points are performed. Adjustment of the light collecting intensity can also be suitably realized.

  FIG. 3 is a block diagram showing an example of the configuration of the light modulation control device 30 applied to the laser light irradiation device 1A shown in FIG. The light modulation control device 30 according to this configuration example includes an irradiation condition acquisition unit 31, a condensing condition setting unit 32, an aberration condition derivation unit 33, a modulation pattern design unit 34, and a light modulator drive control unit 35. Configured. Note that such a light modulation control device 30 can be configured by a computer, for example. The control device 30 is connected to an input device 37 used for inputting information necessary for light modulation control, instructions, and a display device 38 used for displaying information to the operator.

The irradiation condition acquisition unit 31 is an irradiation condition acquisition unit that acquires information related to the irradiation condition of the laser beam on the irradiation target 15. Specifically, the irradiation condition acquisition unit 31 sets the laser light incident pattern (for example, intensity distribution and phase distribution information) to the spatial light modulator 20 as the laser light irradiation condition, from the light modulator 20 to the condensing point. Are the first refractive index n _{1 of} the first propagation medium (for example, atmosphere medium) on the laser light propagation path and the first refractive index of the second propagation medium closer to the condensing point than the first propagation medium. to get a different second refractive index n ₂ (irradiation condition acquiring step).

The condensing condition setting unit 32 is a condensing condition setting unit that sets the condensing condition of the laser beam with respect to the irradiation target 15. Specifically, the condensing condition setting unit 32, as the condensing condition of the laser light, the number s _t of the focal point for irradiating light collecting the modulated laser beam from the spatial light modulator _20, and s _t number of current The condensing position and condensing intensity are set for each of the light spots s (s = 1 to s _t ) (condensing condition setting step). The number s _t of the focal point is set as an integer of 1 or more, also, in the case of multi-point simultaneous irradiation is set as an integer of 2 or more. The acquisition of the irradiation condition by the acquisition unit 31 and the setting of the light collection condition by the setting unit 32 are information prepared in advance in the control device 30, information input from the input device 37, or information supplied from an external device. Based on the above, it is performed automatically or manually by an operator.

  The aberration condition deriving unit 33 derives an aberration condition related to the aberration generated on the propagation path in the propagation of the laser light from the spatial light modulator 20 to the condensing point s set for the irradiation target 15. Deriving means. Here, as described above with reference to FIG. 2, the aberration condition deriving unit 33 includes the first propagation medium on the optical system side having different refractive indexes on the propagation path of the laser light, and the second propagation on the condensing point side. For the medium, an aberration condition caused by the propagation medium is derived (aberration condition deriving step). When there are three or more propagation media on the propagation path, the aberration condition deriving unit 33 derives aberration conditions for all of the propagation media.

  The modulation pattern design unit 34 is a modulation pattern design unit that designs CGH as a modulation pattern to be presented to the spatial light modulator 20 in consideration of the aberration condition on the propagation path derived by the aberration condition deriving unit 33. . Specifically, the modulation pattern design unit 34 refers to the irradiation conditions acquired by the acquisition unit 31, the condensing conditions set by the setting unit 32, and the aberration conditions derived by the derivation unit 33, and those conditions are referred to. Based on the above, a modulation pattern for condensing and irradiating laser light to a desired single or plural condensing points is designed (modulation pattern design step).

  In particular, the modulation pattern design unit 34 in the present embodiment assumes a plurality of pixels that are two-dimensionally arranged for the spatial light modulator 20 in the design of the modulation pattern presented to the spatial light modulator 20, and uses a plurality of pixels. In one pixel of the modulation pattern to be presented (one pixel assumed in the spatial light modulator 20, corresponding to the one pixel when the spatial light modulator 20 has a two-dimensional array of pixels) A design method focusing on the influence of the change of the phase value on the focused state of the laser beam at the focusing point is used. And while changing the phase value of 1 pixel so that the condensing state may approach a desired state, such a phase value change operation is performed about all the pixels (at least all the pixels which light enters) of a modulation pattern. By doing so, an optimal modulation pattern is designed.

In addition, in the modulation pattern design unit 34, when evaluating the condensing state of the laser light at the condensing point in the above-described operation of changing the phase value in each pixel, the pixels in the modulation pattern of the spatial light modulator 20 For the propagation of light from j to the condensing point s, the wave propagation function φ _js in the case of assuming free propagation in a homogeneous state of the propagation medium is not used as it is, but the aberration condition for the propagation function φ _js The propagation function φ _js ′ converted by adding the aberration condition obtained by the deriving unit 33 is used. Thereby, the condensing state of the laser beam is controlled in consideration of the aberration condition on the propagation path.

  The light modulator drive control unit 35 drives and controls the spatial light modulator 20 via the driving device 28 and presents the modulation pattern designed by the modulation pattern design unit 34 to a plurality of pixels of the spatial light modulator 20. Drive control means. Such a drive control unit 35 is provided as necessary when the light modulation control device 30 is included in the laser light irradiation device 1A.

  The processing corresponding to the control method executed in the light modulation control device 30 shown in FIG. 3 can be realized by a light modulation control program for causing a computer to execute light modulation control. For example, the light modulation control device 30 includes a CPU that operates each software program necessary for light modulation control processing, a ROM that stores the software program and the like, and a RAM that temporarily stores data during program execution. And can be configured. In such a configuration, the light modulation control device 30 described above can be realized by executing a predetermined control program by the CPU.

  In addition, the above-described program for causing the CPU to execute each process for light modulation control using the spatial light modulator 20, particularly for designing a modulation pattern presented to the spatial light modulator 20, is recorded on a computer-readable recording medium. Can be recorded and distributed. In such a recording medium, for example, a magnetic medium such as a hard disk and a flexible disk, an optical medium such as a CD-ROM and a DVD-ROM, a magneto-optical medium such as a floppy disk, or a program instruction is executed or stored. For example, hardware devices such as RAM, ROM, and semiconductor non-volatile memory are included.

  The effects of the light modulation control method, the light modulation control program, the light modulation control device 30, and the laser light irradiation device 1A according to the present embodiment will be described.

In the light modulation control method, the control program, and the control device 30 illustrated in FIGS. 1 to 3, with regard to the focused irradiation of the laser light onto the condensing point using the spatial light modulator 20, the incident pattern of the laser light, And information including the refractive indexes of the first and second propagation media on the propagation path, and the number of condensing points s _t of the laser light, and the condensing position and condensing intensity at each condensing point are included. Set the light collection conditions. Then, the aberration condition deriving unit 33 derives an aberration condition caused when the first and second propagation media having different refractive indexes are on the propagation path of the laser light, and the modulation pattern design unit 34 determines the aberration condition. Considering this, a modulation pattern to be presented to the spatial light modulator 20 is designed. Thereby, with respect to the single or plural condensing points set in the condensing condition setting unit 32, in the condensing state of the laser light at each condensing point, the influence of the aberration due to the first and second propagation media is reduced. Can be reduced.

Further, regarding the design of the modulation pattern in such a configuration, specifically, a pixel structure including a plurality of pixels arranged two-dimensionally in the spatial light modulator 20 is assumed. Then, a design method that focuses on the influence of the change of the phase value at one pixel of the modulation pattern on the condensing state of the laser beam at the condensing point is used, and in the evaluation of the condensing state at the condensing point, the propagation medium Instead of using the wave propagation function φ _js when assuming free propagation in a homogeneous state, the condensing state is evaluated after conversion to the propagation function φ _js ′ in which the aberration conditions are considered. According to such a configuration, it is possible to appropriately and reliably evaluate and control the condensing state of the laser light at the condensing point.

  As for the pixel structure assumed in the spatial light modulator 20, when a spatial light modulator having a plurality of two-dimensionally arranged pixels is used as the spatial light modulator 20, the pixel structure is directly used as a modulation pattern. Can be applied to any design. As for free propagation, here, not only propagation in a vacuum or in the atmosphere, but generally propagation in a state where the propagation medium is homogeneous as described above, for example, there is no second propagation medium, and there is no first propagation. It includes propagation when only the medium exists uniformly.

  In the laser beam irradiation apparatus 1A shown in FIG. 1, the laser beam irradiation apparatus 1A is configured by using the laser light source 10, the phase modulation type spatial light modulator 20, and the light modulation control apparatus 30 having the above configuration. ing. According to such a configuration, the control device 30 suitably and surely controls the condensing state of the laser light at the condensing point, and the laser for the single condensing point or the plurality of condensing points set in the irradiation object 15. It is possible to suitably realize operations such as focused irradiation of light and processing and observation of an object by the light. Moreover, such a laser beam irradiation apparatus can be used as a laser processing apparatus, a laser microscope, etc., for example.

Here, with regard to the derivation of the aberration condition in the derivation unit 33, when light propagation from the pixel j to the set condensing point s among the plurality of pixels of the spatial light modulator 20 is considered, It is preferable to obtain a phase Φ _j-OPD that gives an optical path length difference OPD in the propagation as an aberration condition for the propagation of. In this case, the design of the modulation pattern in the design unit 34 uses the phase Φ _j-OPD of the aberration condition derived as described above, and the conversion formula φ _js ′ = φ _js + Φ _j-OPD
Thus, it is preferable to obtain the propagation function φ _js ′ in consideration of the aberration condition. According to such a configuration, the propagation function φ _js of free propagation can be suitably converted into a propagation function φ _js ′ in which the aberration condition is considered.

In addition, regarding the design of the modulation pattern in the design unit 34, the following equation U _s is set, where A _{j-in is the} amplitude of laser light incident on the pixel j of the spatial light modulator 20, and φ _j is the phase value at the pixel j. = A _s exp (iφ _s )
= Σ _j A _j-in exp (iφ _js ') exp (iφ _j )
Thus, it is preferable to obtain the complex amplitude U _s indicating the condensing state at the condensing point s. Or further, the incident amplitude of the laser light to the pixel j of the spatial light modulator 20 _{A j-in,} the injection phase phi _j-in, the phase value of the pixel j as phi _j, the following equation U _s = _{A s} exp (iφ _s )
= Σ _j A _j-in exp (iφ _js ') exp (i (φ _j + φ _j-in ))
Thus, it is preferable to obtain the complex amplitude U _s indicating the condensing state at the condensing point s. Thereby, the condensing state of the laser beam in a condensing point can be evaluated suitably.

Here, the incident amplitude A _j-in of the laser beam to the pixel j is equal to the incident intensity I _j-in .
I _j-in = | A _j-in | ²
Are in a relationship. Further, the complex amplitude _{U s, A s} is the amplitude, phi _s phase. Further, when the incident laser beam is a plane wave, the incident phase φ _j-in can be ignored.

As for the specific configuration of the modulation pattern design, in the change of the phase value at the pixel j of the modulation pattern, the propagation function considering the phase φ _{s of the} complex amplitude indicating the condensing state at the condensing point _s and the aberration condition A configuration in which the phase value is changed based on φ _js ′ and a value analytically obtained based on the phase value φ _j before the change at the pixel j can be used. As a method of updating the phase value analytically in this way, for example, there is an ORA (Optimal Rotation Angle) method.

  Alternatively, in changing the phase value at the pixel j of the modulation pattern, the phase value may be changed by a value obtained by searching using any one of the hill-climbing method, the annealing method, and the genetic algorithm. Here, in the genetic algorithm, operations such as a mutation for selecting one pixel and changing the value of the pixel, and a crossover operation for selecting two pixels and exchanging the value of the pixel are performed. The design method that focuses on the influence of the change in the phase value of one pixel of the pattern on the condensing state of the laser beam at the condensing point includes a method for performing such an operation. The modulation pattern design method will be specifically described later.

  Regarding the first and second propagation media having different refractive indexes on the propagation path of the laser beam, in FIG. 2, the second propagation medium on the condensing point side is an irradiation object whose condensing point is set inside. 15 and the first propagation medium on the optical system side is an atmospheric medium between the spatial light modulator 20 and the irradiation object 15 (between the objective lens 25 and the object 15). Yes. In this case, the atmosphere medium may be water, oil, or the like in addition to air.

  Further, there may be three or more media on the propagation path between the spatial light modulator and the condensing point. As such a configuration, for example, a configuration in which the laser beam passes through a medium having a refractive index different from that of the atmospheric medium, and the laser beam is condensed after passing through the medium is considered. In addition, for example, a configuration in which a plurality of types of glasses having different refractive indexes are laminated, a configuration in which glass is laminated on silicon, and a cover glass is a propagation path for observation of a biological sample or a cell inside a microscope. Various configurations of the medium on the laser light propagation path, such as the configuration existing above, are conceivable. Further, a configuration in which a plurality of media are simultaneously focused and irradiated with laser light is also conceivable. Even in such a case, it is possible to derive the aberration condition and design the modulation pattern in the same manner as described above.

  Further, in the light modulation control device 30 shown in FIG. 3, in addition to the configuration for designing the modulation pattern, the spatial light modulator 20 is driven and controlled, and the modulation pattern designed by the design unit 34 is converted to the spatial light. An optical modulator drive control unit 35 to be presented to the modulator 20 is provided. Such a configuration is effective when the control device 30 is incorporated in the laser light irradiation device 1A as shown in FIG. Further, such a drive control unit 35 may be provided as a separate device from the light modulation control device 30.

  For example, when an optical integrated circuit is manufactured by processing a glass medium by laser light irradiation, one or more new CGHs are designed after one or more times of laser light irradiation. The modulation pattern presented to the spatial light modulator 20 may be switched. Alternatively, when the shape of the optical integrated circuit to be manufactured is determined, a plurality of modulation patterns necessary for laser processing may be designed in advance.

  In addition, when the DOE is used alone, the DOE is a static pattern, so that there is no need for a driving device. In addition, when a pattern is dynamically switched using a plurality of DOEs, a switching device is used instead of the driving device.

  A light modulation control method and a modulation pattern design method executed in the laser light irradiation apparatus 1A and the light modulation control apparatus 30 shown in FIGS. 1 and 3 will be further described along with specific examples thereof. FIG. 4 is a flowchart showing an example of an optical modulation control method executed in the optical modulation control apparatus 30 shown in FIG.

In the control method shown in FIG. 4, first, information about the irradiation condition to the irradiation target 15 of the laser light supplied from the laser light source 10 is acquired (step S101). Specifically, for the propagation path of the laser light from the spatial light modulator 20 to the condensing point s, the first refractive index n _{1 of} the first propagation medium (for example, atmospheric medium) on the propagation path and the second propagation medium (e.g., irradiation target) to obtain a second refractive index _{n 2} of the (S102). Here, if necessary, information other than the refractive indexes of the first and second propagation media, for example, information on the thickness, shape, position, etc. of the media is also acquired. In addition to the propagation medium, if there is information necessary for deriving aberration conditions, such as the NA of the objective lens 25 and the focal length f, it is acquired in addition to the propagation medium information.

Further, an incident pattern of the laser light supplied from the laser light source 10 to the spatial light modulator 20 is acquired (S103). The incident pattern of this laser beam is the incident laser beam intensity I _in (x _j , y _j ) = for the pixel j at the position (x _j , y _j ) in the two-dimensionally arrayed pixels of the spatial light modulator 20 = I _j-in
Is given as the incident light intensity distribution. Or you may acquire the incident pattern of a laser beam as incident light amplitude distribution by amplitude _Aj-in . In addition, if necessary, the configuration may be such that the incident phase φ _j-in of the laser light is also acquired.

Next, a laser beam condensing condition for the irradiation object 15 is set (S104). First, it sets the number s _t of single or multiple focal point for irradiating light collecting a laser light phase-modulated by the spatial light modulator 20 to the irradiation object 15 (S105). Here, in the laser beam irradiation apparatus 1 </ b> A having the above-described configuration, it is possible to obtain a plurality of condensing points as required by the modulation pattern presented to the spatial light modulator 20.

Also, for each of _{s t} number of converging point s = 1 to s _t with respect to the object 15, the condensing position of the laser beam _{γ s = (u s, v} s, z s), and desired condensing intensity I _s-des is set (S106). In addition, about the condensing intensity | strength of the laser beam to each condensing point, you may set not only the setting by the absolute value of an intensity | strength but the relative ratio of an intensity | strength, for example.

  Subsequently, in the propagation of laser light from the spatial light modulator 20 to the condensing point s, aberration conditions caused by the first and second propagation media having different refractive indexes are derived (S107). Then, in consideration of the aberration condition derived in step S107, the laser light irradiation condition and the light collection condition acquired and set in steps S101 and S104 are referred to and presented to a plurality of pixels of the spatial light modulator 20. A CGH to be a modulation pattern is designed (S108).

  The method for deriving the aberration condition executed in step S107 in the flowchart of FIG. 4 will be specifically described. When the spatial light modulator 20 is replaced with a mirror in the configuration shown in FIG. 1, since the phase modulation is not performed on the laser light supplied from the laser light source 10, ideally parallel light enters the objective lens 25, It is converted into a spherical wave by the objective lens 25. When there is no aberration object in the laser light propagation path (condensing path), the light from the objective lens 25 is collected at one point at a condensing depth equal to the focal length f.

  On the other hand, when the first and second propagation media having different refractive indexes are present in the propagation path, an aberration is generated due to a change in the refraction angle, and the light from the objective lens 25 is not condensed at one point. On the other hand, by appropriately designing the modulation pattern presented to the spatial light modulator 20 and deforming the wavefront of the light propagated to the objective lens 25, the aberration of the set condensing point s is reduced. Laser light can be collected without any influence.

For derivation of the wavefront for condensing the laser beam at a desired condensing point, for example, a derivation method based on back ray tracing from a desired condensing position can be used. In the following, a wavefront derivation method for condensing light at a condensing point on the optical axis inside a parallel flat substrate without being affected by aberration will be described as an example (see Patent Document 2). For derivation of the wavefront and derivation of an aberration condition (for example, phase Φ _j-OPD representing an aberration condition described later), for example, an optimization correction method (Non-Patent Document 5) other than the method using reverse ray tracing. Specifically, various methods such as an analysis method for aberrations in paraxial rays (Non-Patent Document 7) can be used.

FIG. 5 is a diagram showing the derivation of the aberration condition that occurs in the propagation of the laser beam. First, consider a case where the refractive index n ₁ of the atmospheric medium is equal to the refractive index n ₂ of the irradiation object 15. When the objective lens 25 is moved to the object 15 side by a distance d on the basis of the position of the objective lens 25 when the light is focused on the position on the end face P of the object 15, the light is only a distance d from the end face P. Condensed to a point O at a distant position. The light incident as an ideal plane wave becomes a spherical wave immediately after being converted by the objective lens 25, and the light beam from the point R in the spherical wave takes the optical path shown by the solid line in FIG. To do. At this time, the optical path length from the point R to the point O is f, and the same optical path length is obtained at any optical axis height.

On the other hand, when the refractive indexes n ₁ and n ₂ are different, the light from the objective lens 25 is not condensed at the point O. Therefore, although the moving amount of the objective lens 25 is the same distance d, the wavefront of the laser light is modulated by the spatial light modulator 20 so as to be condensed at a point O ′ at a position z _s away from the end face P. To do. In this case, the light beam from the point O ′ reaches the point R via the point Q on the boundary surface between the object 15 and the atmospheric medium, and the sum of O′Q and QR becomes the optical path length. Such an optical path length (OPL) is derived for each optical axis height h.

First, as shown in FIG. 5, when the incident angle of the light beam before wavefront correction to the object 15 is θ, the incident angle of the light beam after wavefront correction to the object 15 is θ ₁ , and the refraction angle is θ ₂ , The optical axis heights h ₁ , h ₂ and h are represented by the following formulas (1), (2) and (3), respectively.

Here, the incident angle θ ₁ and the refraction angle θ ₂ are uniquely related by Snell's law. Further, the angles θ, θ ₁ , and θ ₂ are uniquely related by the relational expression h = h ₁ + h ₂ and the above expressions (1) to (3). For example, when a specific θ ₁ or θ ₂ is given, the above formulas (1) and (2) are substituted into the relational expression h = h ₁ + h ₂ to easily solve the formula (3). θ can be determined.

However, it is difficult to analytically obtain θ ₁ and θ ₂ when a specific θ is given. A search is performed when obtaining θ ₁ and θ ₂ corresponding to a specific angle θ. For example, the value of θ ₁ or θ ₂ is gradually changed, and the value of θ is obtained each time. Then, until θ ₁ and θ _{2 at} which θ becomes a desired value are obtained, θ ₁ or θ ₂ is changed to search and derive an angle.

As described above, θ ₁ and θ ₂ corresponding to the desired θ are obtained by the equations (1) to (3). Then, for each incident angle θ, an optical path length OPL of light propagation generated by the irradiation object 15 is obtained by the following equation (4).

Note that “−f− (n ₂ −n ₁ ) × d” in the equation (4) is a constant term, which is a term added to prevent the value of OPL from becoming too large.

This formula (4) shows the optical path length for each incident angle θ. From formula (3) and formula (4), the optical path length for each optical axis height h is as shown in the following formula (5). It can also be expressed as

Thereby, the OPL corresponding to the optical axis height h can be obtained.

The spatial light modulator (SLM) 20 gives this OPL difference, that is, a phase Φ _OPD that gives an optical path length difference (OPD: Optical Path Difference), thereby condensing the laser light at a desired position inside the object 15. be able to. This phase Φ _OPD is given by equation (5)

Can be obtained. This phase Φ _OPD is derived for each z _s with the distance d fixed for three-dimensional multipoint irradiation. The range of the optical axis height h is from 0 to h _max . Further, h _max is in the range of 0 to NA × f, that is, the opening of the objective lens 25 is the maximum of h _max of the optical axis height.

The optical axis height h and the position (x _j , y _j ) of the pixel j of the SLM 20 have the following relationship. When the SLM 20 and the objective lens 25 are imaged by a 4f optical system like the optical system shown in FIG. 1, the wavefront of the objective lens pupil is propagated to the SLM. At this time, when the focal length of the lens 21 of the 4f optical system is f1, and the focal length of the lens 22 is f2, the lateral magnification M is M = f2 / f1. Therefore, the light from the exit pupil of the objective lens has an optical axis height of h = 0 to h _max / M on the SLM.

Further, if it is found that the center position of the light from the exit pupil of the objective lens 25 is at the coordinates (x _c , y _c ) on the SLM, the following equation (7)

Thus, the optical axis height h and the pixel coordinates (x _j , y _j ) of the SLM can be converted. Thereby, the phase Φ _{j-OPD serving} as an aberration condition for each pixel j of the coordinates (x _j , y _j ) can be obtained.

  Next, the modulation pattern design method executed in step S108 of the flowchart of FIG. 4 will be specifically described. In the following, a design method using the ORA method will be described as an example of a design method focusing on the influence of the phase value of one pixel of the modulation pattern presented to the SLM 20 (Patent Document 3, Non-Patent Documents 1 and 2). reference).

  Here, in general, there are a plurality of CGH design methods used as modulation patterns in the SLM, such as an iterative Fourier method. First, the iterative Fourier transform method prepares two surfaces, an SLM surface and a diffraction surface, and propagates between each surface by Fourier transform and inverse Fourier transform. Then, the amplitude information of each surface is replaced for each propagation, and finally the phase distribution is acquired.

  On the other hand, as another CGH design method, there are two methods, a ray tracing method and a design method focusing on the influence of one pixel. As a ray tracing method, there is a lens superposition method (S method: Superposition of Lens). This method is effective when there is little wavefront overlap from the condensing point, but when the wavefront overlap increases, the intensity of light propagating to the condensing point out of the laser light intensity incident on the SLM becomes remarkably high. It may decrease or become uncontrollable. For this purpose, there is an iterative S method that is an improvement of the S method.

  On the other hand, a design method that focuses on the influence of one pixel of CGH is a method in which one pixel of CGH is appropriately selected and the phase value is changed for each pixel to design CGH. Depending on the determination method, there are a search type method and an analysis type method.

  In this design method, the phase value of one pixel with CGH is changed as a parameter, the modulated laser light is propagated using a wave propagation function by Fresnel diffraction or the like, and a value indicating a condensing state at a desired condensing point (for example, Examine how the amplitude, intensity, and complex amplitude values change. Then, a phase value is adopted such that the condensing state at the condensing point approaches a desired result. Such an operation is performed pixel by pixel on at least all the pixels on which light is incident.

  After the operation is completed for all the pixels, the analysis type method returns to the first pixel after confirming how the phase at the desired position changes as a result of the phase modulation of all the pixels. Using the phase at the desired position, the phase is changed pixel by pixel. Further, in the search method, the first pixel is returned without performing confirmation. Examples of the search-type method include a hill-climbing method, an annealing method (SA: Simulated Annealing), and a genetic algorithm (GA: Genetic Algorithm) (see Non-Patent Documents 3 and 4).

The ORA (Optimal Rotation Angle) method described below is an optimization algorithm using an analytical method. In this method, the change and adjustment of the phase value in each pixel of the modulation pattern are performed before the change in the phase φ _{s of the} complex amplitude indicating the condensing state at the condensing point _s , the phase φ _{js of the} propagation function, and the pixel j. This is performed by a value obtained analytically based on the phase value φ _j . In particular, in the design method of this embodiment, as the propagation function, instead of phi _js, first, aberration condition by the second propagation medium by propagation function phi _js' consideration is used.

FIG. 6 is a flowchart showing an example of a modulation pattern design method executed in the light modulation control device 30 shown in FIG. First, the information of the set condensing condition is acquired about the condensing irradiation of the laser beam to the irradiation target 15 performed via the spatial light modulator 20 (step S201). The condensing conditions acquired here include the number of condensing points s _t , the condensing position γ _s of each condensing point _s = (u _s , v _s , z _s ), and the desired condensing intensity I _s. There is _-des .

Next, a phase pattern serving as an initial condition for designing a CGH used as a modulation pattern presented to the SLM 20 is created (S202). This phase pattern is created by, for example, a method in which the phase value φ _j at the pixel j of the CGH is a random phase pattern. This method is used for the purpose of preventing falling into a specific minimum solution due to a random phase because CGH design by ORA is an optimization method. If the possibility of falling into a specific minimum solution can be ignored, a uniform phase pattern or the like may be set, for example.

Subsequently, when the number of the focal point is set to a plurality (s _t ≧ 2), is a parameter for adjusting a condensing intensity ratio between their converging point s = 1 to s _t weights w _s is set to w _s = 1 as the initial condition (S203). In addition, the weight _{w s} is a sequence of 1 × _{s t.} In addition, when there is a single condensing point (s _t = 1), setting of the weight is unnecessary.

When the setting of the phase pattern φ _{j of the} CGH and the weight w _s is completed, a complex amplitude U _s indicating the condensing state of the laser light at the condensing point _s is calculated (S204). Specifically, the following equation (8) representing the light wave propagation

To obtain the complex amplitude U _s = A _s exp (iφ _s ). Here, A _j-in is the incident amplitude of the laser beam to the pixel j of the SLM 20, and φ _j is the phase value at the pixel j. Φ _j-in is the phase of the laser light incident on the pixel j.

In Equation (8), φ _js ′ is a propagation function that takes into account aberration conditions due to the first and second propagation media (atmosphere medium, irradiation object 15 in the example shown in FIG. 5),

Sought by. In this equation (9), Φ _j-OPD is the phase of the aberration condition for the pixel j shown in equation (6).

As described above, by using the propagation function φ _js ′ in which the aberration condition is taken into consideration, it is possible to obtain CGH capable of giving a desired result at any condensing point where z _s is different. Φ _js is a propagation function in a finite region when free propagation is assumed. As this propagation function φ _js , for example, the following equation (10)

Fresnel diffraction, which is an approximate expression of the wave propagation function given by Here, in the above equation (10), k is a wave number.

As the free propagation propagation function φ _js , for example, various derived equations such as the above-described Fresnel diffraction approximation, Fraunhofer diffraction approximation, or the Helmholtz equation can be used. In the above equations (8) and (9), if the phase of the aberration condition is Φ _j−OPD = 0, the propagation function is φ _js ′ = φ _js and is used in the conventional ORA method. The calculation formula of the complex amplitude which does not consider the aberration is obtained.

  Further, when the CGH design by the ORA method is performed using the propagation function of Expression (10), the CGH to which the lens effect of the focal length f of the objective lens is added is designed. However, since the pixel size in SLM is usually large, the lens effect of the objective lens cannot be expressed. For this reason, actually, a value of the focal length L (for example, L = 1m in the case of LCOS-SLM X10468 manufactured by Hamamatsu Photonics) is used instead of the focal length f.

Subsequently, it is determined whether a desired result is obtained in the design of the CGH by the above method (S205). As a determination method in this case, for example, the condensing intensity I _s = | A _s | ² obtained at each condensing point s and the desired intensity I _s-des are expressed by the following equation (11).

And a method of determining whether the intensity ratio is equal to or less than a predetermined value ε at all the condensing points s can be used. Also, rather than collecting light intensity _{I s,} the amplitude _{A s,} determination may be performed by complex amplitude _{U s} like.

  Alternatively, in the flowchart of FIG. 6, a method may be used in which a determination is made based on conditions such as whether a loop such as a change in phase value and calculation of complex amplitude has been performed a prescribed number of times. If it is determined that the designed CGH satisfies the necessary conditions for the set light collection condition, the CGH design algorithm by ORA is terminated. If the condition is not satisfied, the process proceeds to the next step S206.

When it is determined that the condition necessary for the end of the design is not satisfied, first, the value of the weight w _s for adjusting the light collection intensity ratio between the light collection points _s is expressed by the following equation (12).

(S206). Here, the parameter η used for updating the weight w _s in the equation (12) is usually customarily about η = 0.25 to 0.35 in order to prevent the ORA algorithm from becoming unstable. Value is used.

Next, a phase value changing operation is performed for each pixel of the CGH so that the condensing state of the laser light at the condensing point s approaches a desired state (S207). In the analysis-type ORA method, the phase change amount Δφ _j to be added to the phase value φ _j of the pixel j in order to bring the condensed state closer to a desired state is obtained by using the complex amplitude phase φ _s obtained by the equation (8), Using the phase φ _js ′ of the propagation function considering the aberration condition Φ _j-OPD and the phase value φ _j before the update, the following equation (13)

And determined analytically. here,



It is. In this way, the method for analytically obtaining the phase value φ _j has an advantage that the time required for the calculation is shortened compared with a method such as a hill-climbing method for obtaining the phase value by searching.

As for Φ _js used for determining the phase change amount Δφ _j , the following equation (17) is used in the normal ORA method.

However, in the improved ORA method described here, in addition to the change of the propagation function described above, in the calculation of Φ _js in the update of the phase value, an equation that takes into account the phase Φ _j-OPD of the aberration condition ( 16) is used.

When the phase change amount Δφ _j is obtained as described above, the following equation (18) is obtained.

By changing the phase value phi _j in the j-th pixel of the CGH, and updates. Then, it is confirmed whether or not the phase value changing operation has been performed on all the pixels (S208). If the changing operation has not ended, j = j + 1 is set, and the phase value changing operation is executed for the next pixel. On the other hand, if the change operation for all the pixels is completed, it performs the calculation of the complex amplitude U _s, and the evaluation of the condensed state by it back to the step S204. By repeatedly executing such an operation, a CGH having a modulation pattern corresponding to the set condensing condition is created.

As described above, the lens effect of the focal length f of the objective lens is given to the CGH designed by the above method. Therefore, when an objective lens having a focal length f is used, with respect to the phase value φ _{j-res of} CGH obtained as a design result by the ORA method,

Just do it. However,

It is. When the focal length L described above is used instead of f _obj , the expression (20) is also changed from f _obj to L.

  Here, in the correction of aberration when a medium having a different refractive index exists on the propagation path, conventionally, a method for obtaining a correction pattern for aberration and adding the correction pattern to the designed modulation pattern of CGH is used. (For example, refer nonpatent literature 5). As a method for deriving a correction pattern in this case, for example, there are an optimization correction method, an analysis method using paraxial approximation, and an analysis method using reverse ray tracing. The phase opposite to the aberration condition derived from these methods is the aberration correction pattern. However, such a pattern addition method may not function properly as described below.

  That is, in the above-described design method focusing on the influence of one pixel of CGH such as the ORA method, it is possible to perform three-dimensional multi-point irradiation of laser light from a plurality of condensing points with one CGH. When a correction pattern is added to such a CGH as in the prior art, the same aberration correction pattern effect is given to all the condensing points reproduced by the CGH. However, in practice, a plurality of set condensing points may have different positions in the optical axis direction (optical axis depth). In this case, since the influence of the aberration varies depending on the optical axis depth, it is necessary to provide an effect of a different aberration correction pattern for each focal point. That is, in the method of adding the correction pattern to the CGH, only aberration correction at a single optical axis depth can be applied, and there is a possibility that correction of aberrations having different optical axis depths may be insufficient.

  On the other hand, Non-Patent Document 6 discloses a design method using an iterative Fourier method. In such a method, it is necessary to perform an additional process for the CGH design for the three-dimensional multipoint irradiation. In order to reproduce the CGH designed by the usual iterative Fourier method, a lens is required after the SLM. This is because the propagation distance is infinite at the design stage, and control for each optical axis depth (condensing position in the optical axis direction) is not possible.

  In this method, in order to change the optical axis depth, it is necessary to separately add a Fresnel lens pattern to the CGH designed by the iterative Fourier method. Further, in order to realize three-dimensional multi-point irradiation, first, CGH is obtained by the iterative Fourier method for each condensing surface (diffraction surface) on which the condensing point is set, and the depth direction is controlled for each CGH. Add the phase of the Fresnel lens pattern. Thereafter, the CGHs of the plurality of light converging surfaces are added together in the form of complex amplitude, and only the phase is extracted. By this operation, the CGH for three-dimensional multipoint irradiation is designed.

  In addition, when adding a Fresnel lens pattern to the CGH for each condensing surface, by adding an aberration correction pattern for correcting the influence of the medium on the propagation path, it is possible to correct spherical aberration for each condensing surface. However, in such a method, since only the phase is extracted after performing the complex amplitude calculation, there is a problem that the amplitude distribution information is lost and it is extremely difficult to distribute the amplitude to each condensing point.

  On the other hand, according to the above-described CGH design method, it is possible to suitably realize such aberration correction and amplitude distribution to each condensing point. In addition, in such a design method, for example, correction of the influence of a medium having a refractive index different from that of air (or water, oil, etc.), which is an atmospheric medium, on the propagation path, three-dimensional multipoint irradiation, and multiple collections It is possible to design a CGH that simultaneously realizes three intensity adjustments between light spots.

  Effects of aberration correction and the like by the light modulation control device 30 and the laser light irradiation device 1A of the above embodiment will be described together with specific examples thereof. 7 to 9 are diagrams showing examples of laser light irradiation patterns (examples of reproduced images of CGH) by the laser light irradiation apparatus 1A. Here, the laser light is spread by a spatial filter, and the light subjected to phase modulation by the LCOS-SLM that is the spatial light modulator 20 is collected by a lens of f = 800 mm. At this time, a cylindrical lens of f = 200 mm is disposed at a position 700 mm away from the condenser lens. In this example, the cylindrical lens is an aberration object inserted into the condensing optical system.

When a modulation pattern that does not perform correction for an aberration object is used, CGH is not correctly displayed due to the influence of the aberration of the cylindrical lens, as shown in FIG. On the other hand, when an aberration object is corrected by the above-described CGH design method, an aberration-corrected image is observed at a position of z _s = 850 mm from the condenser lens, as shown in FIG.

  The aberration correction for the cylindrical lens is slightly different from the above-described parallel plane substrate in the OPD derivation method and the like. That is, in the case of a parallel plane substrate, since it is axially symmetric, two-dimensional calculation can be used. On the other hand, in the case of a cylindrical lens or when an object has an inclination, it is necessary to perform an appropriate OPD deriving method corresponding thereto.

In addition, since the CGH design method described above has accurate information such as the condensing position including the optical axis depth, the refractive index, and the pixel pitch in the spatial light modulator, the laser beam can be applied to the desired position. Condensation irradiation, laser processing, etc. can be performed. Here, FIG. 9 shows a result of reproducing the CGH for reproducing the “HPK” pattern designed by the normal iterative Fourier method when no object is present in the propagation path. On the other hand, FIG. 8 reproduces and displays a combination of the CGH designed by the ORA method so as to collect light at the position (0, 0, z _s ) on the optical axis and the CGH of the “HPK” pattern. This is the result.

  Comparing FIG. 8 and FIG. 9, it can be seen that the reproduction position in the horizontal direction of the drawing is different. Although the shape of the condensing point is good, the CGH used as the modulation pattern in FIG. 8 is not corrected for the lateral diffraction refracted by the cylindrical lens. On the other hand, there are the following two methods for improving the lateral diffraction.

In other words, the first method is a method of deriving OPD for each reproduction point, including the position of the surface perpendicular to the optical axis direction. In this case, since the position information of the point s is included in Φ _j-OPD , φ _js is common to all the points s, and Φ _j-OPD is different for each position of the point.

The second method is a method of deriving an OPD that differs depending on the optical axis depth without including the position of the surface perpendicular to the optical axis direction. In this case, since the position information of the point s is not included in Φ _j-OPD , φ _js adjusts the position of the plane perpendicular to the optical axis direction, that is, φ _{js corresponds} to the position of each point. Different.

When the latter method is applied and the focal length L is used instead of the actual focal length f as described above, it is necessary to change (u _s , v _s ). Even if f is used or L is used, there is no problem if (u _s , v _s ) is designed correctly in order to finally remove the lens effect. Therefore, when the focal length L is used, (u _s ′, v _s ′) after the change is set to (u _s ′, v _s ′) = (βu _s , βv _s ). Note that β is a parameter for correcting that the focal length of the lens has been changed. When the distance between the optical axis and (u _s , v _s ) is short, β = L / f.

  The CGH is designed using these methods. By doing so, each condensing point can be reproduced at a predetermined position.

  Thus, correctly deriving the aberration amount and designing the CGH has a great effect on the laser beam irradiation position accuracy. In laser light irradiation when the refractive index of the medium is unknown, a method of performing laser light irradiation, confirming the condensing position (for example, processing position), and then performing feedback by changing the refractive index is also considered. It is done.

  The modulation pattern design method executed in step S108 in the flowchart of FIG. 4 will be further described. In the flowchart of FIG. 6, a design method using the analytic ORA method is shown as an example of a design method focusing on the influence of one pixel of CGH. On the other hand, as a modulation pattern design method, as described above, a search-type design method such as a hill climbing method, an annealing method, or a genetic algorithm can be used.

FIG. 10 is a flowchart showing another example of a modulation pattern design method executed in the light modulation control device 30 shown in FIG. In this flowchart, as an example of a search type design method, a design method in the case of using a hill-climbing method is shown. In this method, first, as in the ORA method, information on the set condensing condition is acquired for the condensing irradiation of the laser beam to the irradiation object 15 performed via the SLM 20 (step S301). Next, the phase pattern φ _j of the initial condition of the CGH design presented to the SLM 20 is created as a random phase pattern, for example (S302).

Subsequently, the operation of changing the phase value phi _j of one pixel of the CGH (S303). Further, the complex amplitude U _s = A _s exp (iφ _s ) indicating the condensing state of the laser light at the condensing point s is calculated using the equation (8) including the propagation function φ _js ′ in which the aberration condition is considered. (S304). After the complex amplitude is calculated, the obtained condensing state is determined (S305).

Here, if the amplitude A _s , intensity I _s = | A _s | ² , or complex amplitude U _s approaches a desired value by switching the phase value φ _j of one pixel, the phase value at that time is adopted. To do. In the hill-climbing method, for example, the phase value for each pixel of CGH is switched from 0π (rad) to a predetermined phase value by 0.1π (rad), for example, 2π (rad), and each time the switching is performed, equation (8) Propagation is performed using Then, the phase value at which the intensity of the condensing point s increases most is obtained by searching.

Subsequently, the switching of the phase values phi _j of one pixel is determined whether the confirmed under all conditions (S306), if not go back to step S303. Further, it is determined whether or not an operation such as changing the phase value of one pixel and determining the condensing state has been performed on all pixels (S307). If not, the pixel number is set to j = j + 1 and the process returns to step S303. Necessary operations are performed on the next pixel.

  If necessary operations have been completed for all the pixels, it is determined whether or not a desired result has been obtained in the CGH design (S308). As a determination method in this case, as in the case of the ORA method, for example, a determination method is performed based on whether or not the values of the light collection intensity, amplitude, complex amplitude, and the like obtained at each light collection point are within an allowable range. Can be used. Alternatively, in the flowchart of FIG. 10, a method may be used in which a determination is made based on conditions such as whether or not a loop such as a change in phase value and determination of a focused state has been performed a prescribed number of times. If the necessary conditions are satisfied, the CGH design algorithm is terminated. If the condition is not satisfied, the process returns to step S303 and the search is repeated from the first pixel.

Here, in the examples of the modulation pattern design method described above, the case where the irradiation target 15 is a parallel plane substrate has been described, but in reality, the medium on the light propagation path such as the target 15 is light. It is also conceivable to have an angle α with respect to the axis. When this inclination α is large, astigmatism occurs in addition to spherical aberration. In such a case, the objective lens NA, in addition to the focal length f, the refractive index _{n 1} of the ambient medium, the incident light intensity of the refractive index _{n 2,} and the laser light with respect to SLM irradiation object 15 distribution _{I j-in} Thus, the inclination α of the object 15 is obtained.

In the design example described above, the two-dimensional aberration condition is derived by an analysis method using reverse ray tracing, because spherical aberration is an axially symmetric aberration. On the other hand, when astigmatism occurs due to the inclination α of the medium and the aberration is not axially symmetric, the aberration condition is derived by an appropriate method corresponding to the aberration condition φ _The CGH may be designed using _OPD .

Further, in order to condense the laser light at an arbitrary position as a condensing point, it may be considered that the laser light beam is condensed at a position different from the optical axis. There is no problem when the diffraction angle of the beam is small, but astigmatism occurs in addition to spherical aberration when it is large. In such a case, the beam inclination β is obtained, the aberration condition is derived by an appropriate method corresponding to the above, and the CGH is designed using the obtained aberration condition φ _OPD .

About the desired condensing intensity I _s-des of the laser light at each condensing point s, the light intensity of the material at the irradiation object 15 or the like is taken into consideration, and the intensity I _s-des according to the irradiation depth. an adjustment, i.e., by changing the intensity _{I s-des} in accordance with the irradiation depth _{z s,} may be performed CGH design.

In addition, since the SLM has a periodic pixel structure, the intensity of light diffracted by the spatial frequency of the CGH displayed on the plurality of pixels differs. Therefore, considering such a diffraction intensity, the irradiation position _{(u s, v s),} by changing the intensity _{I s-des} in accordance with the irradiation depth _{z s,} may be performed CGH design.

Further, even when the intensity Is _-des is adjusted as described above, there may be a case where the intensity still varies. In such a case, the laser beam irradiation result, for example, the processing result such as the amount of change in the refractive index generated at the irradiation site is observed, the intensity Is _-des is changed by feedback with reference to the observation result, and the CGH May be designed.

  In addition, in the case where the irradiation object 15 is processed at the condensing point by the focused irradiation of the laser light, the above example illustrates the production of the optical integrated circuit by the internal processing of the glass, but the processing target in the case of performing the laser processing The material of the object 15 is not limited to the glass medium, and various materials such as silicon inside and SiC can be processed.

  Further, in the above embodiment, the laser processing inside the object 15 mainly by the focused irradiation of the laser beam to the irradiation object 15 is described, but the above-described light modulation control device and the modulation pattern are described. The laser beam irradiation apparatus using the design method can be applied to various apparatuses such as a laser microscope such as a laser scanning microscope for cell observation, in addition to the laser processing apparatus.

  FIG. 11 is a diagram showing a configuration of another embodiment of a laser beam irradiation apparatus including a light modulation control apparatus according to the present invention. The laser beam irradiation apparatus 1B according to the present embodiment has the same configuration as that shown in FIG. 1 including the laser light source 10, the movable stage 18, the spatial light modulator 20, the drive device 28, and the light modulation control device 30. However, in addition to these, a detection unit 40, a lens 41, and a dichroic mirror 42 are further provided.

  The dichroic mirror 42 is provided between the lens 22 constituting the 4f optical system and the objective lens 25 in the laser light irradiation optical system. The light from the irradiation target 15 reflected by the dichroic mirror 42 is configured to enter the detection unit 40 via the lens 41.

  As a result, the laser beam irradiation apparatus 1B in FIG. 11 irradiates the observation sample 15 that is the irradiation target with the laser beam, and the detection unit 40 observes the reflected light, scattered light, or fluorescence from the sample 15. It is configured as a scanning microscope. As for the laser scan on the sample 15, in FIG. 11, the sample 15 is moved by the movable stage 18, but a movable mechanism, a galvanometer mirror, or the like may be provided on the optical system side.

FIG. 12 is a diagram illustrating an example of focused irradiation of laser light onto the irradiation target (observation sample) 15 in the laser light irradiation apparatus 1B illustrated in FIG. For example, in cell observation using a cell as the sample 15, as shown in FIG. 12, the shape of the cell may differ depending on the observation position. In such a case, it is necessary to obtain the phase φ _OPD of the aberration condition corresponding to each shape.

Further, in a laser scanning microscope, refractive index mismatching occurs not only during the convergence process of laser light but also during the divergence process during observation. In this case, it is conceivable that the CGH is designed by deriving the aberration condition φ _OPD in consideration of the divergence process, and correction of reflected light, scattered light, fluorescence, etc. is performed using another SLM. Thereby, for example, in a confocal microscope, an improvement in the accuracy of sample observation can be expected.

  Moreover, although the said embodiment demonstrated embodiment about the phase modulation of a single wavelength laser beam, the several laser beam component from the several light source from which a wavelength differs is made to inject into SLM, and wavelength of SLM is made into SLM. A modulation pattern for modulating a plurality of different light components may be displayed to modulate each phase. For example, Non-Patent Document 8 describes a modulation pattern design method for simultaneously modulating a plurality of light components having different wavelengths.

A case where a plurality of wavelengths are controlled using the configuration of the above embodiment will be specifically described. When acquiring the condensing condition information, the condensing position of the point s and the information on the wavelength to be condensed are acquired. Then, the aberration condition φ _OPD is obtained for each point s, and the propagation function φ _js that varies depending on the wavelength and position is converted into φ _js ′ and used.

  The light modulation control method, the control program, the control device, and the laser light irradiation device according to the present invention are not limited to the above-described embodiments and configuration examples, and various modifications are possible. For example, the configuration of the optical system including the laser light source and the spatial light modulator is not limited to the configuration examples shown in FIGS. 1 and 11, and various configurations may be used specifically.

In addition, regarding the design of the modulation pattern (CGH) presented to the spatial light modulator, specifically, various methods other than the above-described examples may be used. In general, in designing a modulation pattern, paying attention to the influence of the change of the phase value at one pixel of the modulation pattern on the condensing state of the laser light at the condensing point, the condensing state approaches the desired state. When designing the modulation pattern by changing the phase value to all the pixels of the modulation pattern and performing the phase value change operation, and evaluating the light collection state at the condensing point, spatial light modulation For the propagation of light from the pixel j to the condensing point s in the modulator modulation pattern, a propagation function φ _js ′ converted by adding an aberration condition to the wave propagation function φ _js of free propagation may be used.

  INDUSTRIAL APPLICABILITY The present invention can be used as a light modulation control method, a control program, a control device, and a laser light irradiation device that can suitably control the condensing state of laser light at a condensing point.

DESCRIPTION OF SYMBOLS 1A, 1B ... Laser beam irradiation apparatus, 10 ... Laser light source, 11 ... Beam expander, 12 ... Reflection mirror, 13 ... Reflection mirror, 15 ... Irradiation target, 18 ... Movable stage, 20 ... Spatial light modulator, 21 ... 4f optical system lens, 22 ... 4f optical system lens, 25 ... objective lens, 28 ... light modulator driving device, 40 ... detection unit, 41 ... lens, 42 ... dichroic mirror,
DESCRIPTION OF SYMBOLS 30 ... Light modulation control apparatus, 31 ... Irradiation condition acquisition part, 32 ... Condensing condition setting part, 33 ... Aberration condition derivation part, 34 ... Modulation pattern design part, 35 ... Light modulator drive control part, 37 ... Input device, 38. Display device.

Claims (17)

A phase modulation type spatial light modulator that inputs laser light, modulates the phase of the laser light, and outputs the laser light after phase modulation is set by the modulation pattern presented to the spatial light modulator. A light modulation control method for controlling the focused irradiation of the laser beam to a focused point,
As the irradiation condition of the laser light, the incident pattern of the laser light to the spatial light modulator, the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point an irradiation condition acquiring step of acquiring a different second refractive index n ₂ than the first refractive index of the second propagation medium in the focal point side than the refractive index n _1, and the first propagation medium,
As the condensing condition of the laser light, the number s _t (s _t is an integer of 2 or more) of the condensing points for condensing and irradiating the laser light from the spatial light modulator, and s _t condensing points. a light collection condition setting step for setting a light collection position and a light collection intensity for each of s;
An aberration condition deriving step for deriving an aberration condition caused by the first propagation medium and the second propagation medium having different refractive indexes in the propagation of the laser light from the spatial light modulator to the condensing point s;
A modulation pattern design step for designing the modulation pattern to be presented to the spatial light modulator in consideration of the aberration condition derived in the aberration condition derivation step;
The modulation pattern design step assumes a plurality of pixels that are two-dimensionally arranged in the spatial light modulator, and a change in phase value at one pixel of the modulation pattern presented to the plurality of pixels is performed at the condensing point. Focusing on the influence of the laser beam on the condensing state, the phase value is changed so that the condensing state approaches a desired state, and such a change operation of the phase value is performed on all the pixels of the modulation pattern. Designing the modulation pattern by performing
When evaluating the condensing state at the condensing point, free propagation in a state where the propagation medium is homogeneous with respect to the light propagation from the pixel j to the condensing point s in the modulation pattern of the spatial light modulator. using the wave propagation function phi _js was converted by the addition of the aberration condition transfer function phi _js',
The aberration condition deriving step obtains a phase Φ _j-OPD that gives an optical path length difference in the propagation as the aberration condition for the light propagation from the pixel j to the condensing point s ,
The modulation pattern design step includes a conversion formula
φ _js ' = φ _js + Φ _j-OPD
Accordingly, the light modulation control method comprising Rukoto determined the propagation function phi _js' that the aberration condition is considered. In the modulation pattern design step, the incident amplitude of the laser beam to the pixel j of the spatial light modulator is A _j-in , the phase is φ _j-in , and the phase value at the pixel j is φ _j , Expression U _s = A _s exp (iφ _s )
= Σ _j A _j-in exp (iφ _js ') exp (i (φ _j + φ _j-in ))
Accordingly, the light modulation control method according to claim 1 Symbol placement and obtaining the complex amplitude U _s indicating the condensing state at the condensing point s. In the modulation pattern design step, in the change of the phase value at the pixel j of the modulation pattern, the phase φ _{s of} complex amplitude indicating the condensing state at the condensing point s and the aberration condition are considered. 3. The light according to claim 1, wherein the phase value is changed according to a value obtained analytically based on a propagation function φ _js ′ and a phase value φ _j before the change at the pixel j. Modulation control method. In the modulation pattern design step, in the change of the phase value at the pixel j of the modulation pattern, the value obtained by the search using any one of a hill-climbing method, an annealing method, or a genetic algorithm is used. 3. The light modulation control method according to claim 1, wherein the phase value is changed. The second propagation medium is an irradiation object in which the condensing point is set inside, and the first propagation medium is an atmospheric medium between the spatial light modulator and the irradiation object. light modulation control method of any one of claims 1-4, characterized in. A phase modulation type spatial light modulator that inputs laser light, modulates the phase of the laser light, and outputs the laser light after phase modulation is set by the modulation pattern presented to the spatial light modulator. A program for causing a computer to execute light modulation control for controlling the focused irradiation of the laser beam to the focused point,
As the irradiation condition of the laser light, the incident pattern of the laser light to the spatial light modulator, the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point and irradiation conditions and acquires a different second refractive index n ₂ than the first refractive index of the second propagation medium in the focal point side than the refractive index n _1, and the first propagation medium,
As the condensing condition of the laser light, the number s _t (s _t is an integer of 2 or more) of the condensing points for condensing and irradiating the laser light from the spatial light modulator, and s _t condensing points. a condensing condition setting process for setting a condensing position and a condensing intensity for each of s;
An aberration condition deriving process for deriving an aberration condition caused by the first propagation medium and the second propagation medium having different refractive indexes in the propagation of the laser light from the spatial light modulator to the condensing point s;
Considering the aberration condition derived in the aberration condition derivation process, causing the computer to execute a modulation pattern design process for designing the modulation pattern to be presented to the spatial light modulator,
The modulation pattern design process assumes a plurality of pixels that are two-dimensionally arrayed in the spatial light modulator, and a change in phase value at one pixel of the modulation pattern presented to the plurality of pixels is performed at the condensing point. Focusing on the influence of the laser beam on the condensing state, the phase value is changed so that the condensing state approaches a desired state, and such a change operation of the phase value is performed on all the pixels of the modulation pattern. Designing the modulation pattern by performing
When evaluating the condensing state at the condensing point, free propagation in a state where the propagation medium is homogeneous with respect to the light propagation from the pixel j to the condensing point s in the modulation pattern of the spatial light modulator. using the wave propagation function phi _js was converted by the addition of the aberration condition transfer function phi _js',
The aberration condition derivation process obtains a phase Φ _j-OPD that gives an optical path length difference in the propagation as the aberration condition for the propagation of light from the pixel j to the condensing point s ,
The modulation pattern design process is a conversion formula
φ _js ' = φ _js + Φ _j-OPD
Accordingly, the light modulation control program characterized Rukoto determined the aberration condition is considered the propagation function phi _js'. In the modulation pattern design process, the incident amplitude of the laser beam to the pixel j of the spatial light modulator is A _j-in , the phase is φ _j-in , and the phase value at the pixel j is φ _j . Expression U _s = A _s exp (iφ _s )
= Σ _j A _j-in exp (iφ _js ') exp (i (φ _j + φ _j-in ))
The light modulation control program according to claim 6 , wherein a complex amplitude U _s indicating the condensing state at the condensing point s is obtained by: In the modulation pattern design process, in the change of the phase value at the pixel j of the modulation pattern, the phase φ _{s of} complex amplitude indicating the condensing state at the condensing point s and the aberration condition are considered. 8. The light according to claim 6 , wherein the phase value is changed according to a value obtained analytically based on a propagation function φ _js ′ and a phase value φ _j before the change at the pixel j. Modulation control program. In the modulation pattern design process, in the change of the phase value at the pixel j of the modulation pattern, the value obtained by the search using any one of the hill-climbing method, the annealing method, or the genetic algorithm is used. 8. The optical modulation control program according to claim 6, wherein the phase value is changed. The second propagation medium is an irradiation object in which the condensing point is set inside, and the first propagation medium is an atmospheric medium between the spatial light modulator and the irradiation object. An optical modulation control program according to any one of claims 6 to 9 . A phase modulation type spatial light modulator that inputs laser light, modulates the phase of the laser light, and outputs the laser light after phase modulation is set by the modulation pattern presented to the spatial light modulator. A light modulation control device for controlling the focused irradiation of the laser beam to the focused point,
As the irradiation condition of the laser light, the incident pattern of the laser light to the spatial light modulator, the first propagation medium on the propagation path of the laser light from the spatial light modulator to the condensing point an irradiation condition acquiring means for acquiring a different second refractive index n ₂ than the first refractive index of the second propagation medium in the focal point side than the refractive index n _1, and the first propagation medium,
As the condensing condition of the laser light, the number s _t (s _t is an integer of 2 or more) of the condensing points for condensing and irradiating the laser light from the spatial light modulator, and s _t condensing points. a condensing condition setting means for setting a condensing position and a condensing intensity for each of s;
An aberration condition deriving unit for deriving an aberration condition caused by the first propagation medium and the second propagation medium having different refractive indexes in the propagation of the laser light from the spatial light modulator to the condensing point s;
Considering the aberration condition derived by the aberration condition deriving means, the modulation pattern design means for designing the modulation pattern to be presented to the spatial light modulator,
The modulation pattern design means assumes a plurality of pixels arranged in a two-dimensional manner in the spatial light modulator, and a change in phase value at one pixel of the modulation pattern presented to the plurality of pixels is performed at the condensing point. Focusing on the influence of the laser beam on the condensing state, the phase value is changed so that the condensing state approaches a desired state, and such a change operation of the phase value is performed on all the pixels of the modulation pattern. Designing the modulation pattern by performing
When evaluating the condensing state at the condensing point, free propagation in a state where the propagation medium is homogeneous with respect to the light propagation from the pixel j to the condensing point s in the modulation pattern of the spatial light modulator. using the wave propagation function phi _js was converted by the addition of the aberration condition transfer function phi _js',
The aberration condition deriving unit obtains a phase Φ _j-OPD that gives an optical path length difference in the propagation as the aberration condition for the light propagation from the pixel j to the condensing point s ,
The modulation pattern design means is a conversion formula
φ _js ' = φ _js + Φ _j-OPD
Accordingly, the light modulation control device according to claim Rukoto determined the aberration condition is considered the propagation function phi _js'. The modulation pattern design unit is configured such that the incident amplitude of the laser beam to the pixel j of the spatial light modulator is A _j-in , the phase is φ _j-in , and the phase value at the pixel j is φ _j . Expression U _s = A _s exp (iφ _s )
= Σ _j A _j-in exp (iφ _js ') exp (i (φ _j + φ _j-in ))
The light modulation control device according to claim 11 , wherein a complex amplitude U _s indicating the light condensing state at the light condensing point s is obtained by: The modulation pattern design means takes into account the phase φ _{s of the} complex amplitude indicating the condensing state at the condensing point s and the aberration condition in changing the phase value at the pixel j of the modulation pattern. 13. The light according to claim 11 , wherein the phase value is changed according to a value obtained analytically based on a propagation function φ _js ′ and a phase value φ _j before the change at the pixel j. Modulation control device. In the change of the phase value at the pixel j of the modulation pattern, the modulation pattern design unit is configured to perform the search according to a value obtained by searching using any one of a hill-climbing method, an annealing method, or a genetic algorithm. 13. The light modulation control apparatus according to claim 11, wherein the phase value is changed. The second propagation medium is an irradiation object in which the condensing point is set inside, and the first propagation medium is an atmospheric medium between the spatial light modulator and the irradiation object. The light modulation control device according to claim 11 , wherein: And driving and controlling the spatial light modulator according to claim, characterized in that it comprises a light modulator drive control means for presenting said modulated pattern designed to said spatial light modulator by said modulation pattern designing means 11-15 The light modulation control device according to claim 1. A laser light source for supplying laser light;
A phase modulation type spatial light modulator that inputs the laser beam, modulates the phase of the laser beam, and outputs the phase-modulated laser beam;
By the modulation pattern to be presented to the spatial light modulator, comprise an optical modulator control device of any one of claims 11 to 16 for controlling the condensing irradiation of the laser light to set the focal point The laser beam irradiation apparatus characterized by this.