R-F DISCHARGE-EXCITED LASER

Abstract: An r-f discharge-excited laser which applies an r-f voltage to a laser tube (1) to generate laser oscillation. The r-f dis­ charge-excited laser comprises an r-f voltage source (12), and a matching circuit (16) for accomplishing the impedance matching between the r-f power source and the laser tube. The connection between reactances (C1, C2) of the matching circuit (16) is connected to the ground potential of the r-f circuit. This makes it possible to decrease change in the laser out­ put caused by mutual current and mutual impedance among the discharge tubes.

Description: Technical Field The present invention relates to a high-frequency discharge pumping laser device for producing a high-power laser beam for cutting workpieces of metal or the like, and more particularly to a high-frequency discharge pumping laser device capable of stable high-frequency discharge pumping. Background Art High-frequency discharge pumping axial-flow CO₂ lasers are finding wide use because of their advantages of high-power output and stable oscillation. A conventional axial-flow-type high-frequency discharge pumping laser device is illustrated in FIG. 9 of the accompanying drawings. The illustrated laser device includes a discharge tube 1 comprising four tube segments. However, the discharge tube 1 may have a desired number of tube segments dependent on the output to be produced. A total reflection mirror 2 and an output coupling mirror 3 are accurately positioned at the ends of the discharge tube 1. Denoted at 4 is an outgoing laser beam. The segments of the discharge tube 1 have gas inlet and outlet ports connected to a single roots blower 7. Cooling units 5, 6 serve to cool a laser gas heated by the discharge and the roots blower 7. The laser gas flows in the discharge tube 1 and gas delivery tubes in the directions of the arrows. Electrodes 8a, 8b ∼ 11a, 11b are connected to respective high-frequency power supplies 12, 13, 14, 15. The gas flows in the discharge tube 1 at the speed of about 100 m/second. An electric discharge is produced in the discharge tube 1 by a high-frequency voltage applied by the high-frequency power supplies 12 ∼ 15 to generate laser oscillation. The circuit arrangement of one discharge tube segment of the conventional high-frequency discharge pumping laser device is shown in FIG. 10. Denoted at 12 is a high-frequency power supply, and 16 a matching circuit for gaining impedance matching between the high-frequency power supply 12 and the discharge tube 1. The output terminals of the high-frequency power supply 12 are coupled to the electrodes 8a, 8b of the discharge tube 1 through the matching circuit 16, the electrode 8b being grounded. With such high-frequency discharge pumping laser device, however, the laser output varies in cyclic periods of about several Hz. Such a laser output fluctuation is illustrated in FIG. 11, with the horizontal axis indicating time and the vertical axis the laser output. As shown in FIG. 11, a laser output fluctuation having the magnitude of about 40 W is produced in the laser output of about 800 W. It is an object of the present invention to provide a high-frequency discharge pumping laser device which will solve the above problem and is capable of stable high-frequency discharge pumping. According to a first aspect of the present invention there is provided a high-frequency discharge pumped laser device comprising a gas discharge laser tube having a plurality of pairs of electrodes and a respective plurality of high-frequency power supplies to produce laser oscillation and respective plural LC matching circuits for impedance matching between the high-frequency power supplies and the laser tube, each matching circuit having a pair of capacitors in series connected across a corresponding pair of electrodes, characterised in that the intermediate point of the capacitors is connected to ground. According to a second aspect of the present invention there is provided a high-frequency discharge pumped laser device comprising a gas discharge laser tube having a plurality of pairs of electrodes and a respective plurality of high-frequency power supplies to produce laser oscillation, and respective plural LC matching circuit for impedance matching between the high-frequency power supplies and the laser tube, characterised in that each matching circuit is isolated from each high-frequency power supply in a DC fashion and is not connected to ground and in that each matching circuit is a balanced circuit. The aforesaid problem arises from a mutual current due to a gas flow between discharge tube segments, and a current due to a mutual impedance of supports supporting the discharge tube segments. According to the first aspect of the present invention, the influences of the mutual current and the mutual impedance are eliminated by grounding the intermediate point of the matching circuit. According to the second aspect of the present invention, the influences of the above currants are eliminated by isolating the matching circuit from the high-frequency power supply in a DC manner. In the drawings:- FIG. 1 is a block diagram of a first embodiment of the present invention; FIG. 2 is a block diagram of a second embodiment of the present invention; FIG. 3 is a block diagram of a third embodiment of the present invention; FIG. 4 is a block diagram of a fourth embodiment of the present invention; FIG. 5 is a block diagram of a fifth embodiment of the present invention; FIG. 6 is a diagram showing a fluctuation of the laser output according to the embodiments of the invention; FIG. 7 is a diagram illustrating an electric current between discharge tube segments; FIG. 8 is a diagram of an equivalent circuit of the arrangement shown in FIG. 7; FIG. 9 is a view showing a conventional axial-flow high-frequency discharge pumping laser device; FIG. 10 is a block diagram of the circuit arrangement of a single discharge tube segment of the conventional high-frequency discharge pumping laser device; and FIG. 11 is a diagram showing a fluctuation of the laser output of the conventional high-frequency discharge pumping laser device. Best Mode for Carrying Out the Invention Embodiments of the present invention will hereinafter be described in specific detail with reference to the drawings. First, interference between discharge tube segments will be described. For the sake of brevity, the discharge tube segments each having two electrodes will be described. FIG. 7 illustrates an arrangement used to explain an electric current between the discharge tube segments. Designated at 1a, 1b are discharge tube segments having electrodes 8a, 8b and 9a, 9b, respectively, to which high-frequency voltages are applied by high-frequency power supplies 12, 13. The reference character A represents a mutual current due to a gas flow between the discharge tube segments 1a, 1b and an impedance of a support supporting the discharge tube 1. An equivalent circuit of the arrangement of FIG. 7 is shown in FIG. 8. Denoted at I₁ is a circuit current from the high-frequency power supply 12 shown in FIG. 7, I₂ a circuit current from the high-frequency power supply 13 of FIG. 7, and I₀ a mutual current between the circuits coupled to the power supplies 12, 13. Designated at Z₀ is a mutual impedance including both a current due to the gas flow and a high-frequency current due to the impedance of the support supporting the discharge tube 1, Z₁₁, Z₁₂ two equal impedances into which the impedance of the discharge tube segment 1a is divided, and Z₂₁, Z₂₂ two equal impedances into which the impedance of the discharge tube segment 1b is divided. Assuming that the voltage and the angular frequency of the high-frequency power supply 12 are indicated by e1 and ω₁, respectively, and the voltage and the angular frequency of the high-frequency power supply 13 are indicated by e2 and ω₂, respectively, with these voltages being expressed by: e1 = E₁sinω₁t e2 = E₂sinω₂t, then the circuit current I₁ is given as follows: I₁ = √ (Ima)² + (Imb)² + 2 ImaImbcosω₃t x sin {ω₄t + tan⁻¹k} where ω₃ = | ω₁ - ω₂| ω₄ = (ω₁ + ω₂)/2 k = (Ima - Imb)/(Ima + Imb) x tan (ω₁ - ω₂)t/2 Ima = E₁ {(Z₂₁ + Z₂₂) (Z₁₂ + Z₀) + Z₂₁Z₂₂}/| Z| Imb = - E₂Z₁₂Z₂₂/| Z| Zm = Z₁₁ + Z₁₂ Zn = Z₂₁ + Z₂₂ Zp = Z₁₂ + Z₂₂ + Z₀ Therefore, by grounding the intermediate point between the power supplies e1, e2, the following equation is obtained: Imb = - E₂Z₁₂(Z₂₁ - Z₂₂)/| Z| Since Z₂₁ and Z₂₂ are generally equal to each other, Imb = 0, and hence I₁ = Ima sinω₁t Ima = E1/(Z₁₁ + Z₁₂) Accordingly, interference between the discharge tube segments 1a, 1b can be prevented by connecting the intermediate point between the power supplies e1, e2 to ground. As can be seen from the equivalent circuit of FIG. 8, the mutual current I₀ flows since the two circuits connected to the respective power supplies have a common grounding circuit. Therefore, the mutual current I₀ does not flow if the grounding circuit is disconnected. This can be achieved by isolating the discharge tube segments from the high-frequency power supplies in a DC manner. FIG. 1 shows in block form a first embodiment of the present invention. In the first embodiment, the intermediate point of a high-frequency power supply is grounded. Denoted at 12 is a high-frequency power supply, and 16 a matching circuit for gaining matching between the high-frequency power supply 12 and a discharge tube 1, the matching circuit 16 comprising inductances L1, L2 and capacitors C1, C2, C3. The matching circuit 16 is a balanced circuit as shown in FIG. 1. Designated at 8a, 8b are electrodes on the discharge tube 1. As described above in detail, the intermediate point between the capacitors C1, C2 is grounded to prevent interference between the discharge tube segments. Since the matching circuit 16 is a balanced circuit, the same result can be achieved by grounding any point on the circuit insofar as the impedance is divided into two equal impedances as viewed from the discharge tube 1 toward the high-frequency power supply 12. FIG. 2 shows a second embodiment of the present invention, which differs from the first embodiment in that the output side of a matching circuit 16 is composed of two capacitors C2, C3. The intermediate point between the capacitors C2, C3 is grounded. As described above, since the matching circuit 16 is a balanced circuit, it can be grounded at either the input or output side thereof. Whether the input side or the output side of the matching circuit 16 is to be grounded may be determined dependent on the packaging conditions for the components of the laser device. FIG. 3 illustrates a third embodiment of the present invention. Denoted at 12 is a high-frequency power supply, and 16 a matching circuit for gaining matching between the high-frequency power supply 12 and a discharge tube 1, the matching circuit 16 comprising an inductance L and capacitors C1, C2, C3. Designated at 8a, 8b are electrodes on the discharge tube 1. As with the first and second embodiments, the intermediate point between the capacitors C1, C2 is connected to ground for preventing interference between the discharge tube segments. However, the matching circuit 16 is an unbalanced circuit. A fourth embodiment shown in FIG. 4 differs from the embodiment of FIG. 3 in that a matching circuit 16 is of an inverted L-shaped configuration. The other details of the fourth embodiment are the same as those of FIG. 3. According to a fifth embodiment shown in FIG. 5, a matching circuit is isolated from a high-frequency power supply in a DC fashion. Denoted at 12 is a high-frequency power supply, and 16 a matching circuit for gaining matching between the high-frequency power supply 12 and a discharge tube 1, the matching circuit 16 comprising inductances L1, L2 and capacitors C1, C2, C3. An isolating transformer T1 isolates the high-frequency power supply 12 and the matching circuit 16 from each other in a DC manner. The matching circuit 16 is a balanced circuit as shown in FIG. 5. Designated at 8a, 8b are electrodes on the discharge tube 1, the electrode 8b being not grounded. With this arrangement, there is no loop in which the mutual current I₀ described above with reference to FIG. 8 would flow, so that current interference between the discharge tube segments is prevented. FIG. 6 is a graph showing the laser output produced by the arrangements illustrated in FIGS. 1, 2, 3, and 4. The graph has a horizontal axis representative of time and a vertical axis of the laser output. As shown in FIG. 6, any variation or fluctuation of the laser output of about 800 W has a magnitude of 10 W or less. Therefore, the laser output fluctuation is reduced as compared with the laser output variation shown in FIG. 11. Substantially the same advantage as that shown in FIG. 6 is obtained by the embodiment of FIG. 5. According to the first invention, as described above, since the intermediate point of the reactance is grounded, interference between the discharge tube segments is eliminated, thus greatly reducing variations or fluctuations of the laser output. According to the second invention, the matching circuit is isolated from the high-frequency power supply in a DC manner to prevent a current from flowing between the discharge tube segments. Consequently, any interference between the discharge tube segments is eliminated. The second invention therefore offers the same advantage as that of the first invention.

Claims: A high-frequency discharge pumped laser device comprising a gas discharge laser tube (1) having a plurality of pairs of electrodes (8a,8b) and a respective plurality of high-frequency power supplies (12) to produce laser oscillation, and respective plural LC matching circuits (16) for impedance matching between the high-frequency power supplies and the laser tube, each matching circuit having a pair of capacitors (C1,C2) in series connected across a corresponding pair of electrodes, characterised in that the intermediate point of the capacitors is connected to ground. A high-frequency discharge pumping laser device according to claim 1, wherein each matching circuit is a balanced circuit, the intermediate point of the reactance of each matching circuit as viewed from said discharge tube being connected to ground. A high-frequency discharge pumped laser device comprising a gas discharge laser tube (1) having a plurality of pairs of electrodes and a respective plurality of high-frequency power (12) supplies to produce laser oscillation, and respective plural LC matching circuit (16) for impedance matching between the high-frequency power supplies and the laser tube, characterised in that each matching circuit is isolated from each high-frequency power supply in a DC fashion and is not connected to ground and in that each matching circuit is a balanced circuit. A high-frequency discharge pumping laser device according to claim 3, wherein each matching circuit (16) is isolated from said high-frequency power supply (12) by a high frequency isolating transformer (T1).

Inventors: EGAWA, AKIRA FANUC MANSION HARIMOMI 3-303
Applicants: FANUC LTD.
Application year: 1988
Main classification: H01S3
IPC codes: H01S3