LASER DEVICE

Abstract: In a laser device a laser beam is produced by a variable-wavelength laser generator which has a Fabry-Perot etalon to select a laser oscillation wavelength, and the laser beam is monitored by a wavelength monitor means whose output sig­ nal is used to adjust a gap pressure of the Fabry-Perot etalon. In order to adjust the gap pressure, the Fabry-Perot etalon is contained in a gas-filled container, and the gas pressure is adjusted by the output signals to tune and stabilize the wave­ length. ABSTRACT A laser apparatus comprising a Fabry-Perot etalon for selecting a laser oscillation wavelength and a wavelength monitor means for monitoring a laser beam taken out from a laser oscillator whose wavelength is variable, whereby the pressure at the gap in the Fabry-Perot etalon is adjusted on the basis of a signal output from the wavelength monitor means. In order to adjust the pressure at the gap the Fabry-Perot etalon is hermetically sealed in a vessel containing a gas and the gas pressure is controlled on the basis of the output signal.

Description: BACKGROUND ART: Fig. 1 is a schematic view showing a conventional wavelength tunable laser apparatus of the type mentioned, for example, in "Applied Optics", July 1974, vol. 13, No. 7, pp. 1625 - 1628. In the figure, the reference numeral 1 denotes a laser oscillator which is, in this case, a dye laser. The numeral 2 denotes a partially reflecting mirror, 3 a Fabry-Perot etalon (hereinafter abbreviated as "FP") provided with a gap, 4 a closed vessel in which the FP 3 is hermetically sealed with a gas, 5 a laser beam, 6 a pressure gauge for measuring the level of gas pressure inside the closed vessel 4, 7 a gas cylinder, 8 valves, and 9 a grating. The operation will next be explained. The laser beam emitted from the laser oscillator 1 has a wavelength selected by various elements incorporated in the oscillator. In this prior art, the range of wavelengths is narrowed by means of spectroscopic elements, that is, the grating 9 and the FP 3, which are inserted in the resonator. Moreover, by adjusting these spectroscopic elements, it is possible to set the wavelength at a desired one within the range of oscillation wavelengths that have been present from the outset. In this prior art, wavelength selection is effected by changing the angle of inclination of the grating 9 and further changing the gas pressure inside the closed vessel 4 to thereby vary the refractive index of the gas in the gap provided in the FP 3. Coarse adjustment of the wavelength can be effected by changing the angle of inclination of the grating 9, and fine adjustment of the wavelength can be achieved by adjusting the gas pressure in the gap of the FP 3. The adjustment of the gas pressure is effected by measuring the level of pressure with the pressure gauge 6 and opening or closing the valves 7 and 8. The conventional laser apparatus which is arranged in the manner described above has the problem that it is necessary to use a pressure gauge which has a degree of accuracy of, for example, better than 0.1% of the full scale in order to perform wavelength tuning with high precision, e.g., tolerances of ±0.001 nm. DISCLOSURE OF INVENTION : The laser apparatus according to the present invention is arranged such that an etalon is hermetically sealed with a gas and the gas pressure is changed with a feedback signal obtained by monitoring the laser beam, thereby effecting wavelength tuning and wavelength stabilization. BRIEF DESCRIPTION OF THE DRAWINGS : Fig. 1 is a schematic view showing a conventional apparatus; Fig. 2 is a block diagram showing one embodiment of the laser apparatus according to the present invention; and Fig. 3 is a chart showing the fringe intensity distribution on the imaging element 22. BEST MODE FOR CARRYING OUT THE INVENTION : One embodiment of the present invention will be described below with reference to the drawings. In Fig. 2, the reference numerals 1 to 4 denote elements which are the same as those of the prior art. The wavelength tuning Fabry-Perot etalon (hereinafter abbreviated as "FP") 3 is accommodated in the closed vessel 4. The reference numeral 10 denotes a totally reflecting mirror which is disposed so as to face the partially reflecting mirror 2 across the FP 4, 11 a volume expanding and contracting means constituted by a bellows which is connected to the closed vessel 4, 12 a mechanism for driving the volume expanding and contracting means 11, 13 a laser beam emitted by the laser oscillator 1 via the totally reflecting mirror 10, the partially reflecting mirror 2 and the FP 3, 14 a beam takeout mirror for taking out a part of the laser beam 13, and 15 a wavelength monitor mechanism which subjects the laser beam taken out by the beam takeout mirror 14 to spectroscopic analysis. The wavelength monitor mechanism 15 comprises an interference filter 16 which passes only the laser beam 13, a filter 17 for adjustment of light intensity, an integrator 18 for diffusing the laser beam 13, an FP 19 for monitoring which is provided with a gap, a closed vessel 20 having the FP 19 hermetically sealed therein, and a lens 21. The numeral 22 denotes an imaging element for observing fringes formed by the FP 19, the imaging element 22 being, for example, a one-dimensional image sensor. The numeral 23 denotes a light-shielding box which contains the elements 16 to 22 and shields them from the ambient light, the light-shielding box 23 being disposed such that the laser beam from the beam takeout mirror 14 can enter the interference filter 16. The numeral 24 denotes a temperature control means for maintaining the temperature of the FP 19 at a constant level, and 25 an image processing means which analyzes the fringes and delivers an output to the driving mechanism 12. The operation will next be explained. The laser beam emitted from the laser oscillator 1 has a wavelength selected by various elements incorporated in the oscillator. In the case of an excimer laser, for example, the range of oscillation wavelengths is originally several angstroms; however, the wavelength range can be narrowed by inserting spectroscopic elements such as a prism, grating, FP, etc. into the resonator. Moreover, by adjusting these spectroscopic elements, it is possible to set the wavelength at a desired one within the range of oscillation wavelengths present from the outset. A part of the laser beam 13 thus obtained is led to the wavelength monitor mechanism 15. The wavelength monitor mechanism 15 employs the FP 19 to determine the wavelength. In the above-described embodiment, circular fringes which appear when light passes through the FP 19 are utilized. The diameter of the fringes is related to ϑ; therefore, the wavelength λ m is determined by obtaining ϑ and utilizing the following expression (1). The FP comprises two mirrors with a high degree of flatness which are disposed so as to face each other across a gap d. Light which passes at an angle of ϑ to the mirror surface has a specific center wavelength which may be expressed as follows: wherein n: the refractive index at the gap m: an integer If an FP having a high resolving power is employed, it is possible to know the intensity of λ m in the laser oscillation wavelength distribution. Since laser beams generally have a certain angle of divergence, only a beam component which satisfies the above expression passes through the FP, thus forming coaxial fringes (ring-shaped interference fringes) around the optical axis of the beam. The wavelength monitor mechanism 15 comprises an integrator 18 which weakens or diffuses the laser beam, an FP 19 and a lens 21. Among the divergent components generated by the integrator 18, only light with ϑ which satisfies the above expression passes through the FP 19 to reach the lens 21. If the focal distance of the lens is assumed to be f, light having a component of ϑ concentrates at a point which is fϑ away from the focal point on the axis of the lens. Accordingly, if the point at which light concentrates is observed by means of the imaging element 22, ϑ is obtained and λ can be calculated. Incidentally, the light intensity distribution on the imaging element 22 is as shown in Fig. 3. The axis of ordinate represents the output, while the axis of abscissa represents the distance x from the center of the fringes. Each peak corresponds to the order m of the FP. The space between each pair of adjacent peaks is called a free spectral range within which a wavelength can be determined uniformly. Moreover, since the free spectral range can be determined by the design of the FP, it is preferable to design it so as to be wider than a value at which a wavelength shift may be expected. Since each peak has a light intensity distribution corresponding to the wavelength distribution of the laser beam, the image processing means 25 is needed to process it so as to obtain ϑ. Further, in this embodiment the present wavelength λ is calculated and the volume expanding and contracting means 11 is activated by the driving mechanism 12 in accordance with the result of the calculation to adjust the level of pressure inside the closed vessel 4, thereby adjusting the wavelength of the oscillator. Although in the above-described embodiment the wavelength monitor mechanism is arranged to measure the fringes formed by the FP by the use of an imaging element, equivalent effects can be obtained by a wavelength monitor mechanism adopting another method. It should be noted that the reason why in the foregoing embodiment the wavelength monitoring FP 19 is not provided in an atmosphere in which a clean gas circulates as in the case of the FP 3 for wavelength selection is that only a part of the laser beam 13 is allowed to enter the FP 19. It is better to provide the FP 19 in an atmosphere in which a clean gas circulates. Although the above-described wavelength monitor means is arranged to measure the fringes formed by the light passing through the FP 19 by means of the fringe imaging element 22, the wavelength may be measured by another method. INDUSTRIAL APPLICABILITY : The present invention is applicable to wavelength stabilization in a laser apparatus, for example, an excimer laser apparatus.

Claims: A laser apparatus comprising: a laser means (1) for generating a laser beam; a first Fabry Perot etalon (3) hermetically sealed with a gas in a closed vessel (4) and having a gas-filled gap wherein changes in the pressure of the gas control the wavelength of the laser beam; and control means (22, 25, 12) for controlling the pressure of the gas, characterized by a wavelength monitoring means (15) which receives a part of the laser beam and determines the wavelength of the laser beam; said control means (22, 25, 12) being responsive to said wavelength monitoring means; and a volume changing means (11) responsive to the control means for changing the pressure of the gas in the gap. The apparatus according to claim 1, characterized in that the wavelength monitoring means comprises a second Fabry Perot etalon (19) having a second gap being disposed in a hermetically sealed vessel (20). The apparatus according to claim 1 or 2, characterized by comprising an integrator (18) for diffusing the laser beam. The apparatus according to one of claims 1 to 3, comprising an imaging element (22) for observing fringes of the second Fabry Perot etalon (19) and image processing means (25) intercoupled between the wavelength monitoring means (15) and the control means, said image processing means generating a signal to control the control means on the basis of the observed fringes.

Inventors: MINOWA YOSHIBUMI MITSUBISHI DE, NAKATANI HAJIME MITSUBISHI DEN, WAKATA HITOSHI MITSUBISHI DENK, MINOWA, YOSHIBUMI MITSUBISHI DENKI K. K., NAKATANI, HAJIME MITSUBISHI DENKI K. K., WAKATA, HITOSHI MITSUBISHI DENKI K. K.
Applicants: MITSUBISHI ELECTRIC CORP, MITSUBISHI DENKI KABUSHIKI KAISHA
Application year: 1988
Main classification: H01S3
IPC codes: H01S3