Title of Invention	METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS
Abstract	When the laser light source is caused to standby, the temperatures of semiconductor laser 1 and semiconductor laser 9 are changed by approximately 3°C from the temperature when the laser light source is always being used. With a temperature change of approximately 3°C, the wavelength of the laser light generated by semiconductor lasers 1 and 9 change approximately 0.3 run. This change hardly has any effect at all on optical fiber amplifier 2 and optical fiber amplifier 10, but the conversion efficiencies at the respective wavelength conversion elements of the wavelength conversion optical system change, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, even while the laser light has been made incident to the wavelength conversion optical system, there is no longer damaging of the wavelength conversion elements. Therefore, it is possible to provide a laser light source standby method that is able to shorten the start up time of the laser light source.

Title of Invention

METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS

Abstract

When the laser light source is caused to standby, the temperatures of semiconductor laser 1 and semiconductor laser 9 are changed by approximately 3°C from the temperature when the laser light source is always being used. With a temperature change of approximately 3°C, the wavelength of the laser light generated by semiconductor lasers 1 and 9 change approximately 0.3 run. This change hardly has any effect at all on optical fiber amplifier 2 and optical fiber amplifier 10, but the conversion efficiencies at the respective wavelength conversion elements of the wavelength conversion optical system change, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, even while the laser light has been made incident to the wavelength conversion optical system, there is no longer damaging of the wavelength conversion elements. Therefore, it is possible to provide a laser light source standby method that is able to shorten the start up time of the laser light source.

Full Text	METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS Technical field [0001] The present invention relates to a method of causing standby (including a method of turning ON and OFF at a high speed) of a laser light source that uses optical fiber amplifiers to perform light amplification of laser light generated from semiconductor lasers and then the forms deep ultraviolet light by means of a wavelength conversion optical system that uses wavelength conversion elements. Background art [0002] Laser light has been used for a variety of applications in recent years, for example, it performs metal cutting and processing, it is used as the light source of photolithography apparatuses in semiconductor fabrication apparatuses, it is used in various measuring apparatuses, and it is used in medical operation and treatment apparatuses such as in surgery, ophthalmology and dentistry. [0003] In the case in which a solid state laser (in the present specification, a semiconductor laser (used as a concept that includes diode lasers)) is used as such a laser light source, the wavelength of the laser light that is emitted from the solid state laser is from the visible range to the infrared range, and a method of directly generating ultraviolet light has not been established. For example, it is not suitable for use in inspecting apparatuses, since the wavelength is too long. Therefore, a method of using such long wavelength light emitted from a solid state laser by converting it into a deep ultraviolet light of a short wavelength (for example, an eighth harmonic: wavelength of 193 nm) by using nonlinear optical crystals has been developed, for example, as described in Japanese Patent Application Publication No. 2001-353176 (Patent Document 1). BBO crystals, LBO crystals and CLBO crystals are known nonlinear optical crystals used for such a purpose. [0004] In an such a laser light source, for example, in general, laser light generated from a DFB-LD is amplified using a plurality of optical fiber amplifiers (FDFA) and is then made into deep ultraviolet light by means of a wavelength conversion optical system such as the above. Patent Document l: Japanese Unexamined Patent Application Publication No. 2001-353176 Disclosure of the Invention Problems to Be Solved by the Invention [0005] Optical fiber amplifiers used for such a purpose, particularly optical fiber amplifiers that amplify light with a wavelength of 1.55 µm to which Er has been added, generate a large amount of heat during high output operations. In addition, when such optical fiber amplifiers are turned ON and OFF, large temperature changes are generated, and, at such times, various unstable statuses are caused. When such optical fiber amplifiers are used in compact packages, the temperature of the housing increases due to the heat generation of the optical fiber amplifiers of subsequent stages of high output operations, and, in conjunction with this, the temperatures of optical fiber of the preceding stages of low output operation, in which heat generation is not performed, also increase. When the temperature of the optical fiber increases, in conjunction with this, the status of polarization of the light output from the optical fiber amplifiers changes. When the status of polarization changes, there is a problem in that the conversion efficiency in the wavelength conversion optical system, into which the output from the optical fiber amplifiers is input, changes, and the laser output light ultimately obtained fluctuates. [0006] Therefore, conventionally, a method has been employed in which, before usage of such a laser light source starts, a warm up of a considerable time is performed, thermal equilibrium is established, fluctuation of the laser output light ultimately obtained is held within an allowable range and then usage is started. However, there are cases in which approximately 24 hours would be necessary until thermal equilibrium is established, and that length of time has been a problem. [0007] As a countermeasure for this, a method in which the laser light source is always put into the output status even while the output light from the laser light source is not being used is conceivable. However, when the laser light source is put into an ON status, the wavelength conversion elements, which are used in the deep ultraviolet light generating portion, or optical elements such as a lenses are damaged, so there is a problem in that maintaining an output status until the time when output light is not used is linked to shortening of the lifespan of the laser light source. As another countermeasure, blocking the laser light using a mechanical shutter before light from the optical fiber amplifiers enters the wavelength conversion optical system is conceivable. However, in this case, the thermal equilibrium of the wavelength conversion optical system breaks down, and, as a result, there is a problem in that fluctuation of the laser output light ultimately obtained cannot be avoided. [0008] The present invention takes such circumstances into account and has as its problem the provision of a laser light source standby method that is able to optically amplify laser light generated from laser oscillating parts using optical fiber amplifiers and then shorten the start up time of a laser light source that performs wavelength conversion by means of a wavelength conversion optical system that uses wavelength conversion elements, as well as a method of turning ON and OFF at a higher speed. Means to Solve Problems [0009] The first means for solving the above problems is a laser light source standby method that causes standby of a laser light source that performs wavelength conversion of laser light generated from laser oscillating parts by means of a wavelength conversion optical system that uses wavelength conversion elements; characterized in that it reduces the wavelength conversion efficiencies of the wavelength conversion elements during standby. [0010] When the wavelength conversion efficiencies of the wavelength conversion elements are reduced, there is a reduction in the output of the converted frequency light that is generated, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, there comes to be extremely little damaging of the wavelength conversion elements by deep ultraviolet light. In changing the laser light source from a standby status to a usage status, a usage status is promptly set by returning the wavelength conversion efficiencies of the wavelength conversion elements to their original settings. [0011] Note that, in the present specification and the Scope of Patent Claims, "reduces the wavelength conversion efficiencies of the wavelength conversion elements" is used with a meaning that includes the case in which they become completely 0. [0012] The second means for solving the above problems is the first means; characterized in that the wavelength-converted laser light is deep ultraviolet light. [0013] The third means for solving the above problems is the first means; characterized in that the method of reducing the wavelength conversion efficiencies of the wavelength conversion elements is setting the temperature that controls the oscillation wavelength of at least one of semiconductor lasers that comprise the laser oscillating parts to a temperature that differs from the temperature of the case in which the laser light source is always being used. [0014] Note that, in the present specification and the Scope of Patent Claims, "the laser light source is always being used" refers to the desired laser light being output from the laser light source. [0015] During standby, when the temperatures of the semiconductor lasers are temperatures different from the temperatures in a case in which the laser light source is always being used, the wavelengths of the laser light (fundamental harmonic) generated from the semiconductor lasers change. Even if this is done, the output of the optical fiber amplifiers is maintained to be nearly constant and enters the wavelength conversion optical system, so thermal equilibrium of the optical fiber amplifiers and the wavelength conversion optical system is maintained at the same level as when a laser light source is used. The output from the optical fiber amplifiers is sent as-is to the wavelength conversion optical system, but wavelength conversion efficiencies drop due to the wavelengths being different, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, there comes to be extremely little damaging of the wavelength conversion elements by deep ultraviolet light. In the case in which there is a shift from a standby status to a usage status, the temperatures of the semiconductor lasers should be returned to their original settings. Temperature changes need only be slight, and the thermal capacities of the semiconductor lasers are small, so the shift from standby to a usage status is promptly performed. [0016] The fourth means for solving the above problems is the first means; characterized in that the method of reducing the wavelength conversion efficiencies of the wavelength conversion elements is to make the temperature of at least one of the temperature-controlled wavelength conversion elements among the wavelength conversion elements temperature that differs from the temperature in the case in which the laser light source is always being used. [0017] When the laser light source is set to a standby status, the temperatures of the wavelength conversion elements are changed from the temperature when the laser light source is always being used. By doing so, the phase matching status of the wavelength conversion elements breaks down, wavelength conversion efficiency drops, and, particularly, deep ultraviolet light is hardly generated at all. Therefore, there comes to be extremely little damaging of the wavelength conversion elements by deep ultraviolet light. In the case in which there is a shift from a standby status to a usage status, the temperatures of the wavelength conversion.elements should be returned to their original settings. Temperature changes need only be slight, and the thermal capacities of the wavelength conversion elements are small, so the shift from standby to the usage status is promptly performed. Particularly, it is preferable that the temperatures of the temperature phase matching crystal used in preceding stages of the wavelength conversion optical system be changed. [0018] The fifth means for solving the above problems is the first means; characterized in that the wavelength conversion elements are nonlinear optical crystals, and the method of reducing the wavelength conversion efficiencies of the wavelength conversion' elements is to make the angle formed by the crystal axes of the nonlinear optical crystals and the optical axis an angle that differs from the angle in the case in which the laser light source is always being used. [0019] The sixth means of solving the above problems is the first means; characterized in that the laser light source is one that optically amplifies laser light using optical fiber amplifiers. [0020] The seventh means for solving the above problems is a method of causing standby of a laser light source that forms deep ultraviolet light from laser light generated from a plurality of laser oscillating parts by means of a wavelength conversion optical system that uses wavelength conversion elements; characterized in that, during standby, the relative relationship of the timing of the pulsed laser light generated from the respective laser oscillating parts is shifted from the relative relationship in the case in which the laser light source is always being used. [0021] In a laser light source that forms deep ultraviolet light from laser light generated from a plurality of laser oscillating parts by means of a wavelength conversion optical system that uses wavelength conversion elements, wavelength conversion is performed by matching the phases of the pulsed laser light generated from these respective laser oscillating parts to the same optical axis and causing them to be incident to the wavelength conversion elements. Therefore, when the relationship of the timing of pulses generated from the respective laser oscillating parts is shifted from the timing in the case in which these laser light sources are always being used, the phases thereof no longer match, the conversion efficiencies of the wavelength conversion elements drop, and, particularly, deep ultraviolet light is hardly generated at all any longer. In the case in which there is a shift from a standby status to a usage status, it is possible to extremely promptly shift to a usage status by making the phases match. [0022] Note that, in the present means, control is performed by shifting the timing of the pulses generated from the laser oscillating parts, so control on the nsec order is possible. Therefore, the time of the "standby" status can be made extremely short, and the concept includes time on the nsec order, for example. Therefore, through the present means, turning ON and OFF in pulsed units, generation of any pulse pattern, and control of pulse energy become possible. [0023] The eighth means of solving the above problems is the seventh means; characterized in that the laser oscillating parts have semiconductor lasers and electrooptical elements (EOMs), and the relative relationship of the timing of the pulsed laser light generated from the respective laser oscillating parts is the relative relationship of the pulsed laser light generated from the semiconductor lasers or the relative relationship of the timing of the pulsqd laser light pulse- extracted by the EOMs. [0024] The ninth means for solving the above problems is the seventh means! characterized in that the laser light source is one that optically amplifies the respective laser lights using optical fiber amplifiers provided to correspond to the respective laser oscillators. Effects of the Invention [0025] Through the present invention, it is possible to provide a laser light source standby method that optically amplifies laser light generated from the laser oscillating parts using optical fiber amplifiers and then shortens start up time of a laser light source that performs wavelength conversion by means of a wavelength conversion optical system that uses wavelength conversion elements, as well as a method of turning ON and OFF at a higher speed. Brief Description of the Drawings [0026] Fig.l Fig. 1 is a drawing that describes the standby method of the laser light source that is the first embodiment of the present invention. Fig. 2 Fig. is a drawing that shows an eighth harmonic pulse waveform when the pulse generation timing has been shifted. Description of Symbols [0027] 1 semiconductor laser 2 optical fiber amplifier 3 condenser lens 4 second harmonic generator 5 condenser lens 6 third harmonic generator 7 condenser lens 8 fifth harmonic generator 9 semiconductor laser 10 optical fiber amplifier 11 condenser lens 12 second harmonic generator 13 condenser lens 14 dichroic mirror 15 condenser lens 16 seventh harmonic generator 17 eighth harmonic generator 18 LD temperature controller 19 LD temperature controller 20 crystal temperature controller 21 crystal temperature controller 22 pulse generator Preferred Embodiment of the Present Invention [0028] Examples of embodiments of the present invention will be described below using drawings. Figure 1 is a drawing that describes the standby method of a laser light source that is an embodiment of the present invention, and it is a drawing that shows an overview of the laser light source. [0029] Laser light (fundamental harmonic) emitted from a first semiconductor laser 1 (DFB-LD) is amplified by a first optical fiber amplifier 2 (FDFA) and is incident to a wavelength conversion optical system. The light that has entered the wavelength conversion optical system is, first, condensed to a second harmonic generator 4 » comprised of LBO by means of a condenser lens 3, and a second harmonic is generated from second harmonic generator 4 along with the fundamental harmonic. These lights are condensed to a third harmonic generator 6 comprised of LBO by means of a condenser lens 5, and a third harmonic is generated from third harmonic generator 6 along with a second harmonic. These lights are condensed to a fifth harmonic generator 8 comprised of BBO by means of a condenser lens 7, and a fifth harmonic is generated from a fifth harmonic generator 8. [0030] On the other hand, laser light (fundamental harmonic) emitted from a second semiconductor laser 9 (DFB-LD) is amplified by a second optical fiber amplifier 10 (FDFA) and is incident to a wavelength conversion optical system. The light that has entered the wavelength conversion optical system"is, first, condensed to a second harmonic generator 12 comprised of LBO via a mirror M by means of a condenser lens 11, and a second harmonic is generated from second harmonic generator 12 along with the fundamental harmonic. These lights pass through a condenser lens 13 and a dichroic mirror 14 and are condensed to a seventh harmonic generator 16 comprised of CLBO. First, a fifth harmonic generated from fifth harmonic generator 8 passes through a condenser lens 15, is reflected by the dichroic mirror 14, and is converged to the seventh harmonic generator 16. A seventh harmonic is generated from seventh harmonic generator 16, but the fundamental harmonic that has entered seventh harmonic generator 16 along with a second harmonic passes through seventh harmonic generator 16 as-is, and a seventh harmonic and the fundamental harmonic are converged to an eighth harmonic generator 17 comprised of CLBO. An eighth harmonic is generated from eighth harmonic generator 17, and this becomes laser light source output. [0031] In the first embodiment, when such a laser light source is caused to standby, the temperatures of semiconductor laser 1 and semiconductor laser 9 are changed by approximately 3°C from the normal temperature (normal temperature is approximately room temperature) when laser light (eighth harmonic) is output from the laser light source (when the laser light source is being used). Semiconductor laser 1 and semiconductor laser 9 are respectively temperature-controlled by LD temperature controllers 18 and 19, so it is possible to easily achieve temperature changes by changing the set temperatures thereof. At a temperature change of approximately 3°C, the wavelengths of the laser light generated from semiconductor lasers 1 and 9 change by approximately 0.3 nm. This change has hardly any effect on optical fiber amplifier 2 and optical fiber amplifier 10, but the conversion efficiencies in the respective wavelength conversion elements of the wavelength conversion optical system are changed, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, the wavelength conversion elements are no longer damaged even while the laser light has been made incident to the wavelength conversion optical system. [0032] When shifting from a standby status to a usage status (a status that outputs laser light (eighth harmonic)), the settings of LD temperature controllers 18 and 19 may be varied to return the temperatures of semiconductor laser 1 and semiconductor laser 9 to their original settings, but only approximately one minute or less is needed until the temperatures are returned to their original settings, so the warm up time can be set to one minute or less. Note that changing of the temperature during standby need not be for both semiconductor laser 1 and semiconductor laser 9, and there will be effects even with only either one of these. [0033] What extent of temperature change should be provided varies according to the wavelength conversion optical system, so, in the wavelength conversion optical system, temperature changes such that deep ultraviolet is no longer generated to the extent of becoming a problem should be experimentally determined and provided. In terms of shortening the warm up time, it is preferable to make the temperature change as small as possible. [0034] In the second embodiment, when such a laser light source is caused to standby, the temperatures of second harmonic generator 4, third harmonic generator 6 and second harmonic generator 12 are changed approximately 1°C from the temperature when the laser light source is always being used. Second harmonic generator 4, third harmonic generator 6 and second harmonic generator 12 are comprised of LBO, which is a temperature phase matching crystal, and they are used for making infrared light into visible light and for making visible light into visible light with a shorter wavelength. These wavelength conversion elements are temperature-controlled (normally 120°C ~ 150°C) by crystal temperature controllers 20, 21, so changing the temperature is easy (note that other wavelength conversion elements are also temperature-controlled, but drawings of the temperature controllers have been omitted). [0035] When the temperature is shifted by approximately 1°C, the phase matching statuses of these temperature phase matching crystals break down, and wavelength conversion efficiency drops. Therefore, generation of deep ultraviolet light greatly drops, and it is possible to prevent damage of wavelength conversion elements 16 and 17, which handle deep ultraviolet light. [0036] When shifting from a standby status to an operation status, the settings of crystal temperature controllers 20 and 21 may be changed to return the temperatures of second harmonic generator 4, third harmonic generator 6 and second harmonic generator 12 to their original settings, but only approximately one minute or less is needed until the temperatures are returned to their original settings, so the warm up time can be set to one minute or less. Note that changing of the temperature during standby need not be for all of second harmonic generator 4, third harmonic generator 6 and second harmonic generator 12, and there will be effects even with only any one or two among these. Even if the temperature of the seventh harmonic generator 16 were changed, there would be effects to a certain extent. However, it is more effective to change the temperature of a harmonic generator of the most preceding stage possible. [0037] What extent of temperature change.should be provided varies according to the wavelength conversion optical system, so, in the wavelength conversion optical system, temperature changes such that deep ultraviolet is no longer generated to the extent of becoming a problem should be experimentally determined and provided. In terms of shortening the warm up time, it is preferable to make the temperature change as small as possible. [0038] In the third embodiment, when such a laser light source is caused to standby, the timing of the pulse generated from semiconductor laser 1 and the timing of the pulse generated from semiconductor laser 9 are shifted by shifting the output timing of a pulse generator 22 that supplies signals to the respective semiconductor lasers 1, 9. In the wavelength conversion optical system, with the timing at which a fifth harmonic formed from the fundamental harmonic generated from semiconductor laser 1 is reflected by the dichroic mirror 14 and is incident to seventh harmonic generator 16 and the timing at which the fundamental harmonic generated from semiconductor laser 9 and a second harmonic formed therefrom pass through the dichroic mirror 14 and are incident to seventh harmonic generator 16 being the same, a second harmonic and a fifth harmonic from among these are superposed, thereby generating a seventh harmonic with good efficiency. When the timing of the pulse generated from this semiconductor laser 1 and the timing of the pulse generated from semiconductor laser 9 are shifted from the usage moving, there is less rsuperposing of a second harmonic and a fifth harmonic or there is no longer superposing at all. Through this, the seventh harmonic generation efficiency drops, or a seventh harmonic is no longer generated. Therefore, deep ultraviolet light generation drops, and there is no damage to seventh harmonic generator 16 and eighth harmonic generator 17. [0039] In returning from a standby status to a usage status, the relative relationship of the pulse generation timing should be returned to its original setting, and it is possible to instantly return to a usage status. Figure 2 is a drawing that shows an eighth harmonic pulse waveform when the pulse generation timing has been shifted in this way. In this case, an eighth harmonic is generated at 500 nsec intervals, but there is a place along the way in which one pulse is missing. This location is a location in which the relative relationship of the pulse generation timing has been shifted from a normal usage status. Specifically, in this case, it is understood that, at 500 nsec, there is a shift from a standby status to a usage status. In addition, if such a method is used, it is also possible to generate any pulse array pattern and to control the energy of the individual pulses. [0040] In addition, electrooptical elements (EOMs) may be respectively arranged in the vicinity of semiconductor laser 1 and semiconductor laser 9, and the timing of extracting pulsed laser lights of the electrooptical elements may also be relatively shifted in order to relatively shift the timing of the pulsed laser light generated from the respective electrooptical elements. The description relating to the wavelength conversion optical system in this case is similar to that of the third embodiment. [0041] In the above, descriptions have been given with respect to three embodiments, but the present invention is one that may be achieved if the wavelength conversion efficiencies of the wavelength conversion elements are reduced by any method. For example, in the case in which the wavelength conversion elements are nonlinear optical crystals, it is possible to realize the present invention even with a method such that the angle formed by the crystal axes thereof and the optical axis is changed.or such that the positional relationship of the respective elements of the wavelength conversion optical system is changed. We claim: 1. A method of controlling a laser light source that generates, in an operation status, deep ultraviolet light from laser light generated from a plurality of laser oscillating parts (1, 9) by means of a wavelength conversion optical system that uses wavelength conversion elements (4, 6, 8, 12, 16, 17), characterized in that the method provides a standby status for the laser light source, during which the wavelength conversion efficiencies of the wavelength conversion elements are reduced compared to the operation status such that deep ultraviolet light is hardly generated at all any longer, wherein reducing the wavelength conversion efficiency during the standby status comprises: setting the temperature that controls the oscillation wavelength of at least one of a plurality of semiconductor lasers (1,9) that comprise the laser oscillating parts (1, 9) to a temperature that differs from the temperature of the respective semiconductor laser during the operation status, or setting the temperature of at least one of a plurality of temperature-controlled wavelength conversion elements among the wavelength conversion elements (4, 6, 8, 12, 16, 17) to a temperature that differs from the temperature of the respective temperature-controlled wavelength conversion element during the operation status, or making the angle formed by the crystal axes of nonlinear optical crystals acting as the wavelength conversion elements and the optical axis an angle that differs from the angle during the operation status, or shifting the relative relationship of the timing of the pulsed laser light generated from the respective laser oscillating parts (1,9) from the relative relationship during the operation status. 2. The method as claimed in claim 1, wherein reducing the wavelength conversion efficiency during the standby status comprises shifting the relative relationship of the timing of the pulsed laser light generated from the respective laser oscillating parts (1,9) from the relative relationship during the operation status, and wherein the laser oscillating parts (1,9) have semiconductor lasers (1, 9) and electrooptical elements, and the relative relationship of the timing of the pulsed laser light generated from the respective laser oscillating parts is the relative relationship of the timing of the pulsed laser light generated from the semiconductor lasers or the relative relationship of the timing of the pulsed laser light pulse extracted by the electrooptical elements. METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS ABSTRACT When the laser light source is caused to standby, the temperatures of semiconductor laser 1 and semiconductor laser 9 are changed by approximately 3°C from the temperature when the laser light source is always being used. With a temperature change of approximately 3°C, the wavelength of the laser light generated by semiconductor lasers 1 and 9 change approximately 0.3 run. This change hardly has any effect at all on optical fiber amplifier 2 and optical fiber amplifier 10, but the conversion efficiencies at the respective wavelength conversion elements of the wavelength conversion optical system change, and, particularly, deep ultraviolet light is hardly generated at all any longer. Therefore, even while the laser light has been made incident to the wavelength conversion optical system, there is no longer damaging of the wavelength conversion elements. Therefore, it is possible to provide a laser light source standby method that is able to shorten the start up time of the laser light source.

Full Text

METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS
Technical field
[0001]
The present invention relates to a method of causing standby (including a method of turning ON and OFF at a high speed) of a
laser light source that uses optical fiber amplifiers to perform light
amplification of laser light generated from semiconductor lasers and
then the forms deep ultraviolet light by means of a wavelength
conversion optical system that uses wavelength conversion elements.
Background art
[0002]
Laser light has been used for a variety of applications in recent
years, for example, it performs metal cutting and processing, it is
used as the light source of photolithography apparatuses in
semiconductor fabrication apparatuses, it is used in various
measuring apparatuses, and it is used in medical operation and

treatment apparatuses such as in surgery, ophthalmology and
dentistry.
[0003]
In the case in which a solid state laser (in the present
specification, a semiconductor laser (used as a concept that includes
diode lasers)) is used as such a laser light source, the wavelength of
the laser light that is emitted from the solid state laser is from the
visible range to the infrared range, and a method of directly

generating ultraviolet light has not been established. For example, it
is not suitable for use in inspecting apparatuses, since the
wavelength is too long. Therefore, a method of using such long
wavelength light emitted from a solid state laser by converting it into
a deep ultraviolet light of a short wavelength (for example, an eighth
harmonic: wavelength of 193 nm) by using nonlinear optical crystals
has been developed, for example, as described in Japanese Patent
Application Publication No. 2001-353176 (Patent Document 1). BBO

crystals, LBO crystals and CLBO crystals are known nonlinear
optical crystals used for such a purpose.
[0004]
In an such a laser light source, for example, in general, laser
light generated from a DFB-LD is amplified using a plurality of
optical fiber amplifiers (FDFA) and is then made into deep ultraviolet
light by means of a wavelength conversion optical system such as the
above.
Patent Document l: Japanese Unexamined Patent Application
Publication No. 2001-353176
Disclosure of the Invention
Problems to Be Solved by the Invention
[0005]
Optical fiber amplifiers used for such a purpose, particularly
optical fiber amplifiers that amplify light with a wavelength of 1.55
µm to which Er has been added, generate a large amount of heat

during high output operations. In addition, when such optical fiber
amplifiers are turned ON and OFF, large temperature changes are
generated, and, at such times, various unstable statuses are caused.
When such optical fiber amplifiers are used in compact packages, the
temperature of the housing increases due to the heat generation of
the optical fiber amplifiers of subsequent stages of high output
operations, and, in conjunction with this, the temperatures of optical
fiber of the preceding stages of low output operation, in which heat
generation is not performed, also increase. When the temperature of
the optical fiber increases, in conjunction with this, the status of
polarization of the light output from the optical fiber amplifiers
changes. When the status of polarization changes, there is a problem
in that the conversion efficiency in the wavelength conversion optical
system, into which the output from the optical fiber amplifiers is
input, changes, and the laser output light ultimately obtained
fluctuates.

[0006]
Therefore, conventionally, a method has been employed in
which, before usage of such a laser light source starts, a warm up of a
considerable time is performed, thermal equilibrium is established,
fluctuation of the laser output light ultimately obtained is held
within an allowable range and then usage is started. However, there
are cases in which approximately 24 hours would be necessary until
thermal equilibrium is established, and that length of time has been
a problem.
[0007]
As a countermeasure for this, a method in which the laser light
source is always put into the output status even while the output
light from the laser light source is not being used is conceivable.
However, when the laser light source is put into an ON status, the
wavelength conversion elements, which are used in the deep
ultraviolet light generating portion, or optical elements such as a

lenses are damaged, so there is a problem in that maintaining an
output status until the time when output light is not used is linked to
shortening of the lifespan of the laser light source. As another
countermeasure, blocking the laser light using a mechanical shutter
before light from the optical fiber amplifiers enters the wavelength
conversion optical system is conceivable. However, in this case, the
thermal equilibrium of the wavelength conversion optical system
breaks down, and, as a result, there is a problem in that fluctuation
of the laser output light ultimately obtained cannot be avoided.
[0008]
The present invention takes such circumstances into account
and has as its problem the provision of a laser light source standby
method that is able to optically amplify laser light generated from
laser oscillating parts using optical fiber amplifiers and then shorten
the start up time of a laser light source that performs wavelength
conversion by means of a wavelength conversion optical system that

uses wavelength conversion elements, as well as a method of turning
ON and OFF at a higher speed.
Means to Solve Problems
[0009]
The first means for solving the above problems is a laser light
source standby method that causes standby of a laser light source
that performs wavelength conversion of laser light generated from
laser oscillating parts by means of a wavelength conversion optical
system that uses wavelength conversion elements; characterized in
that it reduces the wavelength conversion efficiencies of the
wavelength conversion elements during standby.
[0010]
When the wavelength conversion efficiencies of the wavelength
conversion elements are reduced, there is a reduction in the output of
the converted frequency light that is generated, and, particularly,
deep ultraviolet light is hardly generated at all any longer. Therefore,

there comes to be extremely little damaging of the wavelength
conversion elements by deep ultraviolet light. In changing the laser
light source from a standby status to a usage status, a usage status is
promptly set by returning the wavelength conversion efficiencies of
the wavelength conversion elements to their original settings.
[0011]
Note that, in the present specification and the Scope of Patent
Claims, "reduces the wavelength conversion efficiencies of the
wavelength conversion elements" is used with a meaning that
includes the case in which they become completely 0.
[0012]
The second means for solving the above problems is the first
means; characterized in that the wavelength-converted laser light is
deep ultraviolet light.
[0013]

The third means for solving the above problems is the first
means; characterized in that the method of reducing the wavelength
conversion efficiencies of the wavelength conversion elements is
setting the temperature that controls the oscillation wavelength of at
least one of semiconductor lasers that comprise the laser oscillating
parts to a temperature that differs from the temperature of the case
in which the laser light source is always being used.
[0014]
Note that, in the present specification and the Scope of Patent
Claims, "the laser light source is always being used" refers to the
desired laser light being output from the laser light source.
[0015]
During standby, when the temperatures of the semiconductor
lasers are temperatures different from the temperatures in a case in
which the laser light source is always being used, the wavelengths of
the laser light (fundamental harmonic) generated from the

semiconductor lasers change. Even if this is done, the output of the
optical fiber amplifiers is maintained to be nearly constant and
enters the wavelength conversion optical system, so thermal
equilibrium of the optical fiber amplifiers and the wavelength
conversion optical system is maintained at the same level as when a
laser light source is used. The output from the optical fiber
amplifiers is sent as-is to the wavelength conversion optical system,
but wavelength conversion efficiencies drop due to the wavelengths
being different, and, particularly, deep ultraviolet light is hardly
generated at all any longer. Therefore, there comes to be extremely
little damaging of the wavelength conversion elements by deep
ultraviolet light. In the case in which there is a shift from a standby
status to a usage status, the temperatures of the semiconductor
lasers should be returned to their original settings. Temperature
changes need only be slight, and the thermal capacities of the

semiconductor lasers are small, so the shift from standby to a usage
status is promptly performed.
[0016]
The fourth means for solving the above problems is the first
means; characterized in that the method of reducing the wavelength
conversion efficiencies of the wavelength conversion elements is to
make the temperature of at least one of the temperature-controlled
wavelength conversion elements among the wavelength conversion
elements temperature that differs from the temperature in the case
in which the laser light source is always being used.
[0017]
When the laser light source is set to a standby status, the
temperatures of the wavelength conversion elements are changed
from the temperature when the laser light source is always being
used. By doing so, the phase matching status of the wavelength
conversion elements breaks down, wavelength conversion efficiency

drops, and, particularly, deep ultraviolet light is hardly generated at
all. Therefore, there comes to be extremely little damaging of the
wavelength conversion elements by deep ultraviolet light. In the case
in which there is a shift from a standby status to a usage status, the
temperatures of the wavelength conversion.elements should be
returned to their original settings. Temperature changes need only be
slight, and the thermal capacities of the wavelength conversion
elements are small, so the shift from standby to the usage status is
promptly performed. Particularly, it is preferable that the
temperatures of the temperature phase matching crystal used in
preceding stages of the wavelength conversion optical system be
changed.
[0018]
The fifth means for solving the above problems is the first
means; characterized in that the wavelength conversion elements are
nonlinear optical crystals, and the method of reducing the

wavelength conversion efficiencies of the wavelength conversion'
elements is to make the angle formed by the crystal axes of the
nonlinear optical crystals and the optical axis an angle that differs
from the angle in the case in which the laser light source is always
being used.
[0019]
The sixth means of solving the above problems is the first
means; characterized in that the laser light source is one that
optically amplifies laser light using optical fiber amplifiers.
[0020]
The seventh means for solving the above problems is a method
of causing standby of a laser light source that forms deep ultraviolet
light from laser light generated from a plurality of laser oscillating
parts by means of a wavelength conversion optical system that uses
wavelength conversion elements; characterized in that, during
standby, the relative relationship of the timing of the pulsed laser

light generated from the respective laser oscillating parts is shifted
from the relative relationship in the case in which the laser light
source is always being used.
[0021]
In a laser light source that forms deep ultraviolet light from
laser light generated from a plurality of laser oscillating parts by
means of a wavelength conversion optical system that uses
wavelength conversion elements, wavelength conversion is performed
by matching the phases of the pulsed laser light generated from these
respective laser oscillating parts to the same optical axis and causing
them to be incident to the wavelength conversion elements. Therefore,
when the relationship of the timing of pulses generated from the
respective laser oscillating parts is shifted from the timing in the
case in which these laser light sources are always being used, the
phases thereof no longer match, the conversion efficiencies of the
wavelength conversion elements drop, and, particularly, deep

ultraviolet light is hardly generated at all any longer. In the case in
which there is a shift from a standby status to a usage status, it is
possible to extremely promptly shift to a usage status by making the
phases match.
[0022]
Note that, in the present means, control is performed by
shifting the timing of the pulses generated from the laser oscillating
parts, so control on the nsec order is possible. Therefore, the time of
the "standby" status can be made extremely short, and the concept
includes time on the nsec order, for example. Therefore, through the
present means, turning ON and OFF in pulsed units, generation of
any pulse pattern, and control of pulse energy become possible.
[0023]
The eighth means of solving the above problems is the seventh
means; characterized in that the laser oscillating parts have
semiconductor lasers and electrooptical elements (EOMs), and the

relative relationship of the timing of the pulsed laser light generated
from the respective laser oscillating parts is the relative relationship
of the pulsed laser light generated from the semiconductor lasers or
the relative relationship of the timing of the pulsqd laser light pulse-
extracted by the EOMs.
[0024]
The ninth means for solving the above problems is the seventh
means! characterized in that the laser light source is one that
optically amplifies the respective laser lights using optical fiber
amplifiers provided to correspond to the respective laser oscillators.
Effects of the Invention
[0025]
Through the present invention, it is possible to provide a laser
light source standby method that optically amplifies laser light
generated from the laser oscillating parts using optical fiber
amplifiers and then shortens start up time of a laser light source that

performs wavelength conversion by means of a wavelength conversion
optical system that uses wavelength conversion elements, as well as a
method of turning ON and OFF at a higher speed.
Brief Description of the Drawings
[0026]
Fig.l
Fig. 1 is a drawing that describes the standby method of the
laser light source that is the first embodiment of the present
invention.
Fig. 2
Fig. is a drawing that shows an eighth harmonic pulse
waveform when the pulse generation timing has been shifted.
Description of Symbols
[0027]
1 semiconductor laser
2 optical fiber amplifier

3 condenser lens
4 second harmonic generator
5 condenser lens
6 third harmonic generator
7 condenser lens
8 fifth harmonic generator
9 semiconductor laser
10 optical fiber amplifier
11 condenser lens
12 second harmonic generator
13 condenser lens
14 dichroic mirror
15 condenser lens
16 seventh harmonic generator
17 eighth harmonic generator
18 LD temperature controller

19 LD temperature controller
20 crystal temperature controller
21 crystal temperature controller
22 pulse generator
Preferred Embodiment of the Present Invention
[0028]
Examples of embodiments of the present invention will be
described below using drawings. Figure 1 is a drawing that describes
the standby method of a laser light source that is an embodiment of
the present invention, and it is a drawing that shows an overview of
the laser light source.
[0029]
Laser light (fundamental harmonic) emitted from a first
semiconductor laser 1 (DFB-LD) is amplified by a first optical fiber
amplifier 2 (FDFA) and is incident to a wavelength conversion optical

system. The light that has entered the wavelength conversion optical
system is, first, condensed to a second harmonic generator 4
»
comprised of LBO by means of a condenser lens 3, and a second
harmonic is generated from second harmonic generator 4 along with
the fundamental harmonic. These lights are condensed to a third
harmonic generator 6 comprised of LBO by means of a condenser lens
5, and a third harmonic is generated from third harmonic generator 6
along with a second harmonic. These lights are condensed to a fifth
harmonic generator 8 comprised of BBO by means of a condenser lens
7, and a fifth harmonic is generated from a fifth harmonic generator
8.
[0030]
On the other hand, laser light (fundamental harmonic) emitted
from a second semiconductor laser 9 (DFB-LD) is amplified by a
second optical fiber amplifier 10 (FDFA) and is incident to a
wavelength conversion optical system. The light that has entered the

wavelength conversion optical system"is, first, condensed to a second
harmonic generator 12 comprised of LBO via a mirror M by means of
a condenser lens 11, and a second harmonic is generated from second
harmonic generator 12 along with the fundamental harmonic. These
lights pass through a condenser lens 13 and a dichroic mirror 14 and
are condensed to a seventh harmonic generator 16 comprised of CLBO.
First, a fifth harmonic generated from fifth harmonic generator 8
passes through a condenser lens 15, is reflected by the dichroic
mirror 14, and is converged to the seventh harmonic generator 16. A
seventh harmonic is generated from seventh harmonic generator 16,
but the fundamental harmonic that has entered seventh harmonic
generator 16 along with a second harmonic passes through seventh
harmonic generator 16 as-is, and a seventh harmonic and the
fundamental harmonic are converged to an eighth harmonic
generator 17 comprised of CLBO. An eighth harmonic is generated

from eighth harmonic generator 17, and this becomes laser light
source output.
[0031]
In the first embodiment, when such a laser light source is
caused to standby, the temperatures of semiconductor laser 1 and
semiconductor laser 9 are changed by approximately 3°C from the
normal temperature (normal temperature is approximately room
temperature) when laser light (eighth harmonic) is output from the
laser light source (when the laser light source is being used).
Semiconductor laser 1 and semiconductor laser 9 are respectively
temperature-controlled by LD temperature controllers 18 and 19, so
it is possible to easily achieve temperature changes by changing the
set temperatures thereof. At a temperature change of approximately
3°C, the wavelengths of the laser light generated from semiconductor
lasers 1 and 9 change by approximately 0.3 nm. This change has
hardly any effect on optical fiber amplifier 2 and optical fiber

amplifier 10, but the conversion efficiencies in the respective
wavelength conversion elements of the wavelength conversion optical
system are changed, and, particularly, deep ultraviolet light is hardly
generated at all any longer. Therefore, the wavelength conversion
elements are no longer damaged even while the laser light has been
made incident to the wavelength conversion optical system.
[0032]
When shifting from a standby status to a usage status (a status
that outputs laser light (eighth harmonic)), the settings of LD
temperature controllers 18 and 19 may be varied to return the
temperatures of semiconductor laser 1 and semiconductor laser 9 to
their original settings, but only approximately one minute or less is
needed until the temperatures are returned to their original settings,
so the warm up time can be set to one minute or less. Note that
changing of the temperature during standby need not be for both

semiconductor laser 1 and semiconductor laser 9, and there will be
effects even with only either one of these.
[0033]
What extent of temperature change should be provided varies
according to the wavelength conversion optical system, so, in the
wavelength conversion optical system, temperature changes such that
deep ultraviolet is no longer generated to the extent of becoming a
problem should be experimentally determined and provided. In terms
of shortening the warm up time, it is preferable to make the
temperature change as small as possible.
[0034]
In the second embodiment, when such a laser light source is
caused to standby, the temperatures of second harmonic generator 4,
third harmonic generator 6 and second harmonic generator 12 are
changed approximately 1°C from the temperature when the laser
light source is always being used. Second harmonic generator 4, third

harmonic generator 6 and second harmonic generator 12 are
comprised of LBO, which is a temperature phase matching crystal,
and they are used for making infrared light into visible light and for
making visible light into visible light with a shorter wavelength.
These wavelength conversion elements are temperature-controlled
(normally 120°C ~ 150°C) by crystal temperature controllers 20, 21,
so changing the temperature is easy (note that other wavelength
conversion elements are also temperature-controlled, but drawings of
the temperature controllers have been omitted).
[0035]
When the temperature is shifted by approximately 1°C, the
phase matching statuses of these temperature phase matching
crystals break down, and wavelength conversion efficiency drops.
Therefore, generation of deep ultraviolet light greatly drops, and it is
possible to prevent damage of wavelength conversion elements 16 and
17, which handle deep ultraviolet light.

[0036]
When shifting from a standby status to an operation status, the
settings of crystal temperature controllers 20 and 21 may be changed
to return the temperatures of second harmonic generator 4, third
harmonic generator 6 and second harmonic generator 12 to their
original settings, but only approximately one minute or less is needed
until the temperatures are returned to their original settings, so the
warm up time can be set to one minute or less. Note that changing of
the temperature during standby need not be for all of second
harmonic generator 4, third harmonic generator 6 and second
harmonic generator 12, and there will be effects even with only any
one or two among these. Even if the temperature of the seventh
harmonic generator 16 were changed, there would be effects to a
certain extent. However, it is more effective to change the
temperature of a harmonic generator of the most preceding stage
possible.

[0037]
What extent of temperature change.should be provided varies
according to the wavelength conversion optical system, so, in the
wavelength conversion optical system, temperature changes such that
deep ultraviolet is no longer generated to the extent of becoming a
problem should be experimentally determined and provided. In terms
of shortening the warm up time, it is preferable to make the
temperature change as small as possible.
[0038]
In the third embodiment, when such a laser light source is
caused to standby, the timing of the pulse generated from
semiconductor laser 1 and the timing of the pulse generated from
semiconductor laser 9 are shifted by shifting the output timing of a
pulse generator 22 that supplies signals to the respective
semiconductor lasers 1, 9. In the wavelength conversion optical
system, with the timing at which a fifth harmonic formed from the

fundamental harmonic generated from semiconductor laser 1 is
reflected by the dichroic mirror 14 and is incident to seventh
harmonic generator 16 and the timing at which the fundamental
harmonic generated from semiconductor laser 9 and a second
harmonic formed therefrom pass through the dichroic mirror 14 and
are incident to seventh harmonic generator 16 being the same, a
second harmonic and a fifth harmonic from among these are
superposed, thereby generating a seventh harmonic with good
efficiency. When the timing of the pulse generated from this
semiconductor laser 1 and the timing of the pulse generated from
semiconductor laser 9 are shifted from the usage moving, there is less
rsuperposing of a second harmonic and a fifth harmonic or there is no
longer superposing at all. Through this, the seventh harmonic
generation efficiency drops, or a seventh harmonic is no longer
generated. Therefore, deep ultraviolet light generation drops, and

there is no damage to seventh harmonic generator 16 and eighth
harmonic generator 17.
[0039]
In returning from a standby status to a usage status, the
relative relationship of the pulse generation timing should be
returned to its original setting, and it is possible to instantly return
to a usage status. Figure 2 is a drawing that shows an eighth
harmonic pulse waveform when the pulse generation timing has been
shifted in this way. In this case, an eighth harmonic is generated at
500 nsec intervals, but there is a place along the way in which one
pulse is missing. This location is a location in which the relative
relationship of the pulse generation timing has been shifted from a
normal usage status. Specifically, in this case, it is understood that,
at 500 nsec, there is a shift from a standby status to a usage status.
In addition, if such a method is used, it is also possible to generate

any pulse array pattern and to control the energy of the individual
pulses.
[0040]
In addition, electrooptical elements (EOMs) may be respectively
arranged in the vicinity of semiconductor laser 1 and semiconductor
laser 9, and the timing of extracting pulsed laser lights of the
electrooptical elements may also be relatively shifted in order to
relatively shift the timing of the pulsed laser light generated from
the respective electrooptical elements. The description relating to the
wavelength conversion optical system in this case is similar to that of
the third embodiment.
[0041]
In the above, descriptions have been given with respect to three
embodiments, but the present invention is one that may be achieved
if the wavelength conversion efficiencies of the wavelength
conversion elements are reduced by any method. For example, in the

case in which the wavelength conversion elements are nonlinear
optical crystals, it is possible to realize the present invention even
with a method such that the angle formed by the crystal axes thereof
and the optical axis is changed.or such that the positional
relationship of the respective elements of the wavelength conversion
optical system is changed.

We claim:
1. A method of controlling a laser light source that generates, in an operation
status, deep ultraviolet light from laser light generated from a plurality of laser
oscillating parts (1, 9) by means of a wavelength conversion optical system that
uses wavelength conversion elements (4, 6, 8, 12, 16, 17), characterized in that
the method provides a standby status for the laser light source, during which the
wavelength conversion efficiencies of the wavelength conversion elements are
reduced compared to the operation status such that deep ultraviolet light is hardly
generated at all any longer, wherein reducing the wavelength conversion
efficiency during the standby status comprises:
setting the temperature that controls the oscillation wavelength of
at least one of a plurality of semiconductor lasers (1,9) that comprise the
laser oscillating parts (1, 9) to a temperature that differs from the
temperature of the respective semiconductor laser during the operation
status, or
setting the temperature of at least one of a plurality of
temperature-controlled wavelength conversion elements among the
wavelength conversion elements (4, 6, 8, 12, 16, 17) to a temperature that
differs from the temperature of the respective temperature-controlled
wavelength conversion element during the operation status, or
making the angle formed by the crystal axes of nonlinear optical
crystals acting as the wavelength conversion elements and the optical axis
an angle that differs from the angle during the operation status, or
shifting the relative relationship of the timing of the pulsed laser
light generated from the respective laser oscillating parts (1,9) from the
relative relationship during the operation status.
2. The method as claimed in claim 1, wherein reducing the wavelength
conversion efficiency during the standby status comprises shifting the relative
relationship of the timing of the pulsed laser light generated from the respective
laser oscillating parts (1,9) from the relative relationship during the operation
status, and wherein the laser oscillating parts (1,9) have semiconductor lasers (1,
9) and electrooptical elements, and the relative relationship of the timing of the
pulsed laser light generated from the respective laser oscillating parts is the
relative relationship of the timing of the pulsed laser light generated from the
semiconductor lasers or the relative relationship of the timing of the pulsed laser
light pulse extracted by the electrooptical elements.

METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY
STATUS

ABSTRACT

When the laser light source is caused to standby, the temperatures of semiconductor laser 1
and semiconductor laser 9 are changed by approximately 3°C from the temperature when
the laser light source is always being used. With a temperature change of approximately
3°C, the wavelength of the laser light generated by semiconductor lasers 1 and 9 change
approximately 0.3 run. This change hardly has any effect at all on optical fiber amplifier 2
and optical fiber amplifier 10, but the conversion efficiencies at the respective wavelength
conversion elements of the wavelength conversion optical system change, and, particularly,
deep ultraviolet light is hardly generated at all any longer. Therefore, even while the laser
light has been made incident to the wavelength conversion optical system, there is no longer
damaging of the wavelength conversion elements. Therefore, it is possible to provide a laser
light source standby method that is able to shorten the start up time of the laser light source.

METHOD FOR HAVING LASER LIGHT SOURCE IN STANDBY STATUS

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