JP2005101482A - Laser device and method for driving same - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To obtain a method for driving a laser device which can store the pulse waveform of a stable single peak in time. <P>SOLUTION: A plurality of Q switches 4 and 5 are arranged in a resonator, and each high frequency modulation signal generated by each high frequency modulation signal generating means 6 and 7 is inputted on the basis of a control signal corresponding to each Q switch generated by a control signal generating means 8 which is common to those Q switches 4 and 5, and the diffraction action of each Q switch element is controlled to execute pulse driving. A laser device is configured to measure an operation delay time corresponding to the control signal of each Q switch 4 and 5, and when any one of those Q switches is used as a reference, the operation delay time of the other Q switch is canceled, and an adjustment time based on the operation delay time measured for each control signal of each Q switch is set so that the operations can relatively be made in-phase. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

  The present invention relates to a laser device and a driving method of the laser device, and more particularly to a laser device in which a plurality of Q switch elements are arranged in a resonator and a driving method thereof.

  A conventional Q-switch type laser device has an apparatus configuration as disclosed in FIG. In the laser oscillator of the conventional laser apparatus shown in FIG. 1 of Patent Document 1, the total reflection mirror and the output mirror are installed to function as a resonator mirror at a position facing a cavity including the YAG crystal and its excitation source system. Has been. On the optical axis in the resonator formed by the total reflection mirror and the output mirror, the first A / O element is disposed on the total reflection mirror side, and the second A / O element is disposed on the output mirror side. Each A / O element is individually connected to a high frequency modulation signal generator, and each high frequency modulation signal generator is further connected to a common control signal generator. The A / O element refers to an acousto-optic element and is a kind of Q switch element.

  The A / O element is composed of a vibrator and, for example, quartz. When quartz is vibrated at a high frequency using the vibrator, ultrasonic waves are transmitted into the quartz. This ultrasonic wave forms a refractive index density in the quartz, and the quartz acts as a diffraction grating. Accordingly, the optical path of the laser beam incident at an incident angle θ in the quartz through which the ultrasonic wave generated by the external high-frequency modulation signal is transmitted is bent by 2θ due to the diffraction action caused by the acoustooptic effect. On the other hand, the laser beam has a property of going straight in quartz where ultrasonic waves are not transmitted. Utilizing this diffraction action, it becomes possible to resonate the laser light between the total reflection mirror and the exit mirror, or to suppress the resonance, thereby serving as a Q switch element.

  Next, a conventional laser device driving method will be described with reference to FIG. In FIG. 2 of Patent Document 1, C1 and Mrf1 indicate a control signal and a high-frequency modulation signal for the first A / O element, and C2 and Mrf2 indicate a control signal and a high-frequency modulation signal for the second A / O element. Also, n (t) represents the time variation of the inversion distribution, P (t) is the pulse laser waveform, n∞ is the limit value of the inversion distribution, ni is the maximum value of the inversion distribution, nf is the minimum value of the inversion distribution, nt Represents the threshold value of the inversion distribution.

  When the first A / O element is turned off from the state in which the control signal C1 is applied, the first A / O element is released from the high-frequency modulation signal Mrf1 that has been applied so far. That is, the high frequency modulation signal generator stops applying the high frequency modulation signal Mrf1 to the first A / O element. By stopping the application, the diffraction effect of the first A / O element disappears, and the light in the cavity can pass through the first A / O element.

  On the other hand, when the control signal C2 for the second A / O element is turned off after a lapse of the predetermined delay time Δt in the control signal generator, the second A / O element is released from the high-frequency modulation signal Mrf2 that has been applied so far. That is, the high frequency modulation signal generation unit stops applying the high frequency modulation signal Mrf2 to the second A / O element. By stopping the application, the light in the cavity can be transmitted through the second A / O element.

  When the second A / O element is released from the high-frequency modulation signal Mrf2, the resonator loss is reduced, stimulated emission in the resonator is started, and pulsed laser light is generated. That is, when the inversion distribution n (t) starts to decrease, the pulse laser beam intensity P (t) starts to increase and reaches the peak intensity when the inversion distribution threshold nt is reached, and then the pulse laser intensity P (t ) Decreases.

  Next, the high frequency modulation signal Mrf1 is applied again to the first A / O element to increase the resonator loss, and as a result, the pulse laser beam disappears. That is, since the stimulated emission is suppressed by diffracting the optical axis in the first A / O element, the inversion distribution n (t) is increased by continuous excitation to the YAG crystal.

  Accordingly, since the pulse width tp of the pulse laser beam is determined according to the time ΔT in which the first A / O element and the second A / O element are simultaneously released from the high frequency modulation signal, the interval between the high frequency modulation signal Mrf1 and the high frequency modulation signal Mrf2 is determined. The pulse width tp of the pulsed laser beam can be controlled by arbitrarily changing the delay time, in other words, Δt, which is the delay time between the control signal C1 and the control signal C2, and even if the pulse repetition frequency is increased, the pulse width tp It was possible to have a constant narrow value.

Japanese Patent Application Laid-Open No. 11-97783

  In the conventional laser apparatus, for example, when the excitation input is increased, the problem that the pulse laser waveform has a plurality of peaks instead of a single peak often occurs. In such a pulsed laser waveform including two or more pulses, the peak position varies with time. In particular, the pulse peak output is reduced and fluctuates over time, with the result that the average output is reduced, and as a result, the processing quality of the laser processing machine is deteriorated.

  The present invention has been made to solve such a problem, and maintains a time-stable single peak pulse waveform to suppress a decrease in pulse peak output and consequently a decrease in average output. It is an object of the present invention to obtain a laser apparatus and a driving method of the laser apparatus that can provide a quality laser processing machine.

  The laser device driving method according to the present invention is based on a control signal corresponding to each Q switch element generated by a control signal generating means common to each Q switch element in which a plurality of Q switch elements are arranged in a resonator. A method of driving a laser device in which each high frequency modulation signal generated by each high frequency modulation signal generating means is inputted and the diffraction action of each Q switch element is controlled to drive a pulse, and the operation of each Q switch element with respect to the control signal Corresponding to each Q switch element in order to make the operation of each Q switch element in phase by eliminating the operation delay time of each other Q switch element with the step of actually measuring the delay time and any one Q switch element as a reference Setting an adjustment time based on the operation delay time measured for each control signal.

  The laser device according to the present invention includes a resonator including a pair of output mirrors and a total reflection mirror, a laser medium disposed on the optical axis in the resonator, and the optical medium in the resonator. One or more Q switch elements arranged between the laser medium and the output mirror and between the laser medium and the total reflection mirror, a position adjusting mechanism provided for each Q switch element, and each Q switch element A plurality of high frequency modulation signal generating means for inputting high frequency modulation signals, respectively, and a control signal generating means provided in common to each of the high frequency modulation signal generating means.

  In the laser device driving method according to the present invention, since the operation delay time for the control signal of each Q switch element is measured in advance and the time adjustment between the control signals is performed, each Q switch element is relatively completely in phase. Therefore, it is possible to drive the laser device so that a time-stable single peak pulse waveform can be maintained and a decrease in pulse peak output and, in turn, a decrease in average output can be suppressed.

  Further, in the laser apparatus according to the present invention, the position of the Q switch element is finely adjusted by the position adjustment mechanism based on the operation delay time with respect to the control signal of each Q switch element. Therefore, it is possible to easily obtain a high-performance laser apparatus capable of holding a pulse waveform having a single peak that is stable in time and suppressing a decrease in pulse peak output and, in turn, a decrease in average output.

Embodiment 1 FIG.
The inventor of the present invention first considered the cause of the above problems. FIG. 1A shows a configuration diagram of the laser device to be considered, and FIG. 1B shows a cavity portion in the configuration of the laser device. In FIG. 1, 1 is a cavity, 2 is a total reflection mirror, 3 is an exit mirror, 4 is a first A / O element (first Q switch element), 5 is a second A / O element (second Q switch element), 6, 7 Denotes a high-frequency modulation signal generator (high-frequency modulation signal generator), and 8 denotes a control signal generator (control signal generator). The function of each component is almost the same as that of a conventional laser device.

  Reference numeral 15 denotes a solid rod, which corresponds to the laser medium in the cavity 1 of FIG. 1A, and a solid rod represented by an Nd: YAG crystal is an example. Reference numerals 16 to 19 denote A / O elements (Q switch elements) described on page 466 of “Solid-State Laser Engineering” by Walter Koechner, for example, in the first and second A / O elements 4 and 5 in FIG. Equivalent to. 16 is an ultrasonic transducer that is the output destination of the high-frequency modulation signals Mrf1 and Mrf2, 17 is an absorber, 18 is quartz glass, 19 is the traveling direction of the ultrasonic wave, 20 is a guide laser for oscillation, and 21 is a guide laser 20 Reference numeral 22 denotes a laser beam, 22 denotes a power meter, and 23 denotes an excitation source.

  In the above-described laser device, for example, when the round trip gain per cavity is an operation under a high gain of 2.8 or more, the diffraction efficiency is 30% or more per A / O element and the fall time of the diffraction loss. Operate by the conventional driving method under various conditions such as 160nsec or less, the number of A / O elements arranged per cavity is 2 or more, the average laser output is 200W or more, the pulse repetition frequency is 6kHz or less, etc. In this case, a pulse laser beam having two or more peaks is included.

  In the laser apparatus of FIG. 1, the control signal C1, the high-frequency modulation signal Mrf1, the control signal C2 of the second A / O element 5, the high-frequency modulation in the first A / O element 4 in the conventional driving method when the excitation input is increased. FIG. 2 shows time changes of the signal Mrf2 and the laser output. In the laser pulse generated as a result of increasing the excitation input, as described above, for example, a pulse waveform including two or more pulses is formed and fluctuates with time. In particular, the phenomenon that the pulse peak output decreased and the time fluctuated frequently occurred.

  This phenomenon is caused by a high excitation input, so that even if a high frequency modulation signal is input to any one of the A / O elements in the cavity 1 and a diffraction action occurs, the state in which laser oscillation occurs is maintained. The inventors of the present invention have found that this occurs.

  In view of such a consideration, the inventor of the present invention has come up with the idea that the above problem can be solved if a plurality of A / O elements are driven in complete synchronization with the control signals C1 and C2 in phase. However, as a result of the experiment, even if the control signals C1 and C2 are set in phase, an operation time delay occurs between the elements due to the diffraction action of each A / O element, and one of the A / O elements is It has been found that the problem of laser oscillation during operation is still unresolved.

  When the inventor of the present invention further advanced the experiment and consideration on the cause of the time delay of the operation between the A / O elements, the following knowledge was obtained.

  When the total reflection mirror 2 and the emission mirror 3 are adjusted so that the laser output is maximized while monitoring the power meter 22 in the laser device described above, for example, a plurality of excitation sources 23 are arranged on the side of the solid rod 15. In this case, the excitation distribution in the solid rod 15 in the direction of the oscillation optical axis 14 has non-axial symmetry reflecting the variation of each excitation source due to variations in wavelength, output, and beam quality at each excitation source.

  Therefore, the oscillation optical axis 14 is passed through the place with the highest excitation density. Even if the guide light 21 is simply made to coincide with the central axis of the solid rod 15, the oscillation optical axis 14 does not coincide with the optical axis of the guide light 21. Therefore, it is not clear that the oscillation optical axis 14 passes through the A / O element unless the oscillation adjustment is performed, and the position through which the oscillation optical axis passes in each A / O element is different. I understood.

  Therefore, regarding the signal arrival time difference (operation delay time) from the control signal generator 8 to the oscillation optical axis 14 in each A / O element shown in FIG. 1A, the input control signal C1 of the high frequency modulation signal generators 6 and 7 is used. , Even if the operation timing of the output high-frequency signals Mrf1 and Mrf2 with respect to C2 is adjusted to zero, for example, the laser beam is caused by the difference in the arrival time of the ultrasonic wave from the ultrasonic transducer 16 to the actual oscillation optical axis 14 in the A / O element. The time variation of the diffraction loss with respect to the A / O element is not completely in phase. This aspect is shown in FIG.

The transmission speed of the sound wave used in the quartz glass 18 as the A / O element is about 6 × 10 ⁶ mm / sec. In such a case, the oscillation optical axis position in the A / O elements 4 and 5 is, for example, 0. It shifts about 5mm. For this reason, the time change of the diffraction loss in the A / O elements 4 and 5 is shifted by about 80 nesc. In the above laser apparatus configuration, since the round trip gain in the oscillator is large, the time required for light growth from when the inversion distribution reaches the oscillation threshold until the laser output reaches the peak value, that is, the build-up time is A / It becomes the same as the fall time of the diffraction loss in the O element, and immediately after the diffraction loss starts to fall, the inversion distribution starts to fall and light starts to grow.

  Furthermore, since the differential coefficient regarding the fall in the resonator loss in one resonator has two values for the reason described above, two inflection points appear at the fall of the inversion distribution, and the time change of the laser output is For example, a pulse waveform including two pulses is formed. In addition, as shown in FIG. 4, the pulse waveform of the laser output varies with time as the operation is repeated.

  The operation timing of the output high-frequency modulation signals Mrf1 and Mrf2 with respect to the input control signals C1 and C2 in the high-frequency modulation signal generators 6 and 7 often shifts by several hundred nsec due to factors such as individual differences in the high-frequency modulation signal generators. Therefore, the time variation in the resonator loss, inversion distribution, and laser output is as shown in FIG. As described above, the time change of the laser output forms, for example, a pulse waveform including two pulses. Further, such an operation causes a decrease in pulse peak output, a time variation, and a decrease in average output, which in turn results in deterioration of processing quality in the laser processing machine.

  As a result of conducting a number of experiments based on the above consideration, the inventor has stabilized the laser device while maintaining the pulsed laser beam having a single peak that does not include two pulses. I came to find a way to drive. Hereinafter, a method for driving the laser apparatus of the present invention, more specifically, a method for adjusting a relative time delay in element operation of each A / O element will be described.

  FIG. 6 is a configuration diagram of a laser apparatus for explaining a method for adjusting the relative time delay of element operation in each A / O element. A laser light detection element 10 and an output monitor 9 are added to the laser device shown in FIG.

  In the laser device driving method according to the first embodiment of the present invention, the control signals C1 and C2 to the first A / O element 4 and the second A / O element 5 are basically set in phase. However, as described above, due to the configuration of the laser device, even if the control signals C1 and C2 are in phase, the A / O elements 4 and 5 do not operate relatively completely in phase due to various factors. Therefore, as will be described below, after measuring the deviation (operation delay time) of the operation timing of each A / O element 4 and 5 with respect to the control signal generated in each laser device, each A / O element is operated during actual laser device operation. The relative time delay between the O elements is adjusted.

  As a first step, a trigger signal, which is a test signal, is generated from the control signal generator 8 and a high frequency modulation signal T1 is applied to the first A / O element (first Q switch element) 4, while the second A / O element It is assumed that the high frequency modulation signal T1 is not input to the (second Q switch element) 5. As a result, the peak value 12 of the pulse laser beam received by the laser beam detection element 10 appears on the output monitor 9. As shown in FIG. 7, a time difference τ 1 between the peak value 12 of the pulse laser beam and the trigger signal obtained from the control signal generator 8 is measured by the output monitor 9. In the actual operation of the laser apparatus, the time difference τ1 means a time difference from when the control signal is generated to when a diffraction loss due to an effective diffraction action occurs in the first A / O element 4 due to the high frequency modulation signal. The value varies between / O elements and individual laser devices.

  As a second step, a trigger signal, which is a test signal, is generated from the control signal generator 8 and a high frequency modulation signal T2 is applied to the second A / O element 5, while a high frequency modulation is applied to the first A / O element 4. It is assumed that the signal T2 is not input. As a result, the peak value 12 of the pulse laser beam received by the laser beam detection element 10 appears on the output monitor 9. Similar to the first step, the time difference τ 2 between the peak value 12 of the pulse laser beam and the trigger signal obtained from the control signal generator 8 is measured by the output monitor 9. In actual operation of the laser apparatus, the time difference τ2 means a time difference from when a control signal is generated until an effective diffractive action is generated in the second A / O element 5 by a high-frequency modulation signal. Or different values between individual laser devices.

  As a third step, the magnitude relationship between the time differences τ1 and τ2 obtained in the first and second steps is determined.

  As a fourth step, when the above-described time differences τ1 and τ2 have a relationship of τ1> τ2, the operation timing of the control signal C2 is set to be delayed by τ1−τ2 with respect to the control signal C1, When the time differences τ1 and τ2 have a relationship of τ1 ≦ τ2, the operation timing of the control signal C1 is effectively delayed in advance by τ2−τ1 with respect to the control signal C2 to generate each control signal. Each control signal C1 ′, C2 ′ is set in advance. This is because the operation of each A / O element, that is, the time change of the diffraction loss is made relatively completely in phase by the effective control signals C1 'and C2'.

That is, the effective control signals C1 ′ (t) and C2 ′ (t) after adjusting the time delay relative to the control signals C1 (t) and C2 (t) before the setting are
(1) When τ1> τ2 C1 ′ (t) = C1 (t)
C2 ′ (t) = C1 (t + (τ1−τ2))
(2) When τ1 ≦ τ2 C1 ′ (t) = C2 (t + (τ2−τ1))
C2 ′ (t) = C2 (t)
The relationship is established.

  By the above-described method, the relative time delay in the operation of the other A / O element when one of the plurality of A / O elements is used as a reference is regarded as the deviation of the operation timing with respect to the reference A / O element. For example, if the control signal C1 is set in advance so as to eliminate the relative time delay with the control signal C2, it is possible to align the element operation in each A / O element, that is, the time variation of the diffraction loss in phase. .

  FIG. 8 shows the time variation of diffraction loss when each A / O element is operated based on the effective control signals C1 ′ and C2 ′ of each A / O element 4 and 5 in the laser apparatus adjusted by the above method. Shown in As can be seen from the figure, the time variation of the diffraction loss of each A / O element was adjusted so that the relative time delay that originally existed between the two became zero. The gap disappears.

  When the laser device is driven based on the control signals C1 'and C2', the resonator loss, the inversion distribution, and the time change of the laser output in the resonator are as shown in FIG. That is, since the relative operation timing shift between the first A / O element 4 and the second A / O element 5 is eliminated, there is no transitional state in which only one A / O element is operated in advance. Only pulsed laser light having a single peak is generated. As a result, it is possible to take out a single pulse that is stable in time, and it is possible to suppress a decrease in pulse peak output and a decrease in average output, thereby realizing high-quality laser processing. .

Embodiment 2. FIG.
In the laser device driving method according to the first embodiment, the time between the control signals C1 and C2 is adjusted. However, in the laser device according to the second embodiment, each A / O is devised based on the configuration of the laser device. Relative time delay between elements is eliminated. FIG. 10 is a diagram illustrating a configuration of a main part of the laser device according to the second embodiment. In the figure, 24 is a position adjusting mechanism for finely adjusting the amount of movement when the A / O element is moved in a direction substantially perpendicular to the direction of the oscillation optical axis 14, and 25 is an A / O by the position adjusting mechanism 24. The movement direction of each element is shown.

When the time differences τ1 and τ2 described in the first embodiment have a relationship of τ1> τ2, the transmission speed of the sound wave in the quartz glass 18 is set to Vp, and the first A / O element 4 is moved by the position adjusting mechanism 24.
X = Vp × (τ1-τ2)
Is moved in the direction of the arrow 25 (oscillation optical axis side) by the movement amount of. When the relationship of τ2> τ1 is satisfied, the second A / O element 5 is moved by the position adjusting mechanism 24.
X = Vp × (τ2−τ1)
Is moved in the direction of the arrow 25 (oscillation optical axis side) by the movement amount of.

  By the above-described method, for example, the second A / O element 5 is moved in the direction of the arrow 25 by the position adjusting mechanism 24 so that the relative time delay of the second A / O element 5 with respect to the first A / O element 4 is eliminated. If the translation is performed by the distance set by the above, it is possible to align the element operation timing between the A / O elements, that is, the time variation of the diffraction loss in phase.

  The time change of the diffraction loss when each A / O element in the laser apparatus adjusted by the above method is operated is the same as that shown in FIG. Similar to the first embodiment, the time variation of the diffraction loss of each A / O element is adjusted so that the relative time delay that originally existed between them becomes zero. The shift is eliminated.

  When the laser device adjusted based on the above-described method is driven, the resonator loss, the inversion distribution, and the time change of the laser output in the resonator are as shown in FIG. As in the first embodiment, the operation timing shift between the first A / O element 4 and the second A / O element 5 is eliminated, so that only one A / O element operates in advance. Since the state disappears, only pulsed laser light having a single peak is generated. As a result, it is possible to take out a single pulse that is stable in time, and it is possible to suppress a decrease in pulse peak output and an average output, thereby realizing high-quality laser processing. It becomes.

  In the laser device and the driving method thereof in each of the above embodiments, the configuration in which one Q switch element is disposed between the laser medium and the output mirror and between the laser medium and the total reflection mirror has been described as an example. It is not limited, and two or more Q switch elements may be arranged, and two or more Q switch elements are arranged either between the laser medium and the output mirror or between the laser medium and the total reflection mirror. Also good.

  In the laser apparatus and the driving method thereof in each of the above-described embodiments, not only the above-described A / O element but also a Q-switch element using an electro-optic effect or a Q-switch element using a mechanical mechanism can be applied. Needless to say. Needless to say, the laser medium can be applied not only to a solid medium but also to a liquid or gas medium.

(A) is a structure of a laser apparatus, (b) is the figure which showed the structure of the cavity part in a laser apparatus. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 3 is an operation explanatory diagram according to the first embodiment. 1 is a configuration diagram of a laser device in Embodiment 1. FIG. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 3 is an operation explanatory diagram according to the first embodiment. FIG. 5 is a configuration diagram of a laser device in a second embodiment.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Cavity, 2 Total reflection mirror, 3 Output mirror, 4 1st A / O element, 5 2nd A / O element, 6 High frequency modulation signal generation part, 7 High frequency modulation signal generation part, 8 Control signal generation part, 9 Output monitor, DESCRIPTION OF SYMBOLS 10 Laser light detection element, 11 Trigger signal, 12 Peak value, 14 Oscillation optical axis, 15 Solid rod, 16 Ultrasonic transducer, 17 Absorber, 18 Quartz glass, 19 Ultrasonic traveling direction, 20 Guide laser, 21 Guide light , 22 Power meter, 23 Excitation source, 24 Position adjustment mechanism, 25 A / O element moving direction.

Claims (10)

A plurality of Q switch elements are arranged in a resonator, and each high frequency modulation signal generating means generated by each high frequency modulation signal generating means based on a control signal corresponding to each Q switch element generated by a control signal generating means common to each Q switch element. A method of driving a laser device that inputs a modulation signal and controls the diffraction action of each of the Q switch elements to drive the laser device,
Measuring an operation delay time of each Q switch element with respect to the control signal;
Measured for each control signal corresponding to each Q switch element in order to eliminate the operation delay time of each other Q switch element and make the operation of each Q switch element in phase with any one Q switch element as a reference Setting an adjustment time based on the operation delay time;
A method for driving a laser device comprising: A plurality of Q switch elements are arranged in a resonator, and each high frequency modulation signal generating means generated by each high frequency modulation signal generating means based on a control signal corresponding to each Q switch element generated by a control signal generating means common to each Q switch element. A method of driving a laser device that inputs a modulation signal and controls the diffraction action of each of the Q switch elements to drive a pulse.
The high frequency modulation signal T1 generated by the high frequency modulation signal generation means is applied to the first Q switch element by a trigger signal from the control signal generation means to cause a diffraction effect, while the second Q switch element has the high frequency modulation signal T1. Receiving a pulse laser beam emitted from the laser device in a state in which the laser beam is not input by a laser beam detection element, and measuring a time difference τ1 between the trigger signal generation time and the pulse laser beam reception time;
A high-frequency modulation signal T2 generated by the high-frequency modulation signal generation means is applied to the second Q switch element by a trigger signal from the control signal generation means to cause a diffractive action, while the high-frequency modulation is applied to the first Q switch element. Receiving a pulsed laser beam emitted from the laser device in a state where the signal T2 is not input by the laser beam detecting element, and measuring a time difference τ2 between the time when the trigger signal is generated and the pulsed laser beam receiving time;
Determining the magnitude of the time differences τ1 and τ2,
When the time differences τ1 and τ2 have a relationship of τ1> τ2, the operation timing of the control signal C2 input to the second Q switch element is set to the time of τ1−τ2 with respect to the control signal C1 input to the first Q switch element. On the other hand, when the time differences τ1, τ2 have a relationship of τ1 ≦ τ2, the control signal C1 is delayed so that the operation timing of the control signal C1 is delayed by τ2-τ1 with respect to the control signal C2. , C2 time adjustment,
A method for driving a laser device comprising: 3. The method of driving a laser device according to claim 1, wherein the Q switch element is constituted by an acousto-optic element. 3. The method of driving a laser device according to claim 1, wherein the Q switch element is constituted by an electro-optical element or an element by a mechanical mechanism. 3. The laser device driving method according to claim 1, wherein the laser medium in the laser oscillator of the laser device is a solid medium. A resonator composed of a pair of output mirrors and a total reflection mirror;
A laser medium disposed on the optical axis in the resonator;
A plurality of Q switch elements disposed on an optical axis in the resonator;
A position adjusting mechanism provided in at least one of the Q switch elements;
A plurality of high frequency modulation signal generating means for inputting a high frequency modulation signal for each of the Q switch elements;
Control signal generating means provided in common for each of the high frequency modulation signal generating means;
A laser device comprising: The laser apparatus according to claim 6, wherein a moving direction of the Q switch element by the position adjusting mechanism is a direction substantially orthogonal to an optical axis of the resonator. The laser apparatus according to claim 6, wherein an amount of movement of the position adjusting mechanism is determined based on an operation delay time of each Q switch element. The operation delay time between the Q switch elements is
A high frequency modulation signal generated by the high frequency modulation signal generation means is applied to one Q switch element by a trigger signal from the control signal generation means to generate a diffractive action, while the other Q switch element has the high frequency modulation signal. Applying a method for measuring the time difference between the trigger signal generation time and the pulse laser beam reception time by receiving the pulse laser beam emitted from the laser device with the laser beam detection element in a state where the laser beam is not input for each Q switch element 9. The laser device according to claim 8, wherein the operation delay time is obtained. Each Q switch element comprises a first A / O element installed between the total reflection mirror and the laser medium, and a second A / O element installed between the output mirror and the laser medium,
Each operation delay time of the first and second Q switch elements is respectively
The high-frequency modulation signal T1 generated by the high-frequency modulation signal generation means is applied to the first Q switch element by the trigger signal from the control signal generation means to cause a diffractive action, while the second Q switch element has the high-frequency modulation signal T1. A time difference τ1 between a trigger signal generation and a pulsed laser beam receiving time measured by receiving a pulsed laser beam emitted from the laser device in a state in which the laser beam is not input by a laser beam detection element,
A high-frequency modulation signal T2 generated by the high-frequency modulation signal generation means is applied to the second Q switch element by a trigger signal from the control signal generation means to cause a diffractive action, while the high-frequency modulation is applied to the first Q switch element. The time difference τ2 between the time when the trigger signal is generated and the time when the pulse laser beam is received is measured by receiving the pulse laser beam emitted from the laser device with the laser beam detecting element in a state where the signal T2 is not input. The laser device according to claim 8.

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