Efficient and compact short pulse MOPA system for laser-produced-plasma extreme-UV sources employing RF-discharge slab-waveguide CO2 amplifiers

Recent studies of fundamental issues of target material format and laser radiation parameters have revealed the attractiveness of LPP EUV source technology based on Sn target and multi-kW CO2 laser driver. In recent work we have reported 8kW of average power at 100kHz repetition frequency and 20ns pulse duration produced by our MOPA CO2 laser driver built on a chain of Fast Axial Flow (FAF) amplifiers. However, the oscillator power is insufficient to saturate the input stages and significant amount of available laser energy (>80%) is untapped. In this paper we report a step towards an improvement of laser driver power and efficiency. For the first time, to our knowledge, the performance of a novel multi-pass pre-amplifier based on RF-excited slab waveguide CO2 laser technology has been numerically modeled. The calculations show the feasibility of this approach. We carried out amplification experiments to validate the numerical model. In our experiments we have obtained power gain of 10 at 13-pass configuration from a slab of 60x600mm2 geometry at 20ns pulse length and 100kHz repetition frequency at diffraction-limited output and no self-oscillation. The experiment has validated the numerical model, which will be used at this stage to design and optimize a pre-amplifier for our current FAF amplifier chain. Furthermore, these results enable us to design and optimize next generation of LPP laser driver based entirely on compact slab-waveguide amplifiers.

[1]  A. Giesen,et al.  Power scalability of thin disk lasers in fundamental mode operation , 2005, CLEO/Europe. 2005 Conference on Lasers and Electro-Optics Europe, 2005..

[2]  Walter Koechner,et al.  Solid-State Laser Engineering , 1976 .

[3]  Akira Endo,et al.  LPP EUV light source employing high power C02 laser , 2008, SPIE Advanced Lithography.

[4]  E. Shcherbakov New achievements in development of superpower industrial fiber lasers and their applications , 2005, CLEO/Europe. 2005 Conference on Lasers and Electro-Optics Europe, 2005..

[5]  R. Simpson,et al.  Multi-kW near-diffraction-limited single-frequency Nd:YAG laser , 2005, CLEO/Europe. 2005 Conference on Lasers and Electro-Optics Europe, 2005..

[6]  Wolfgang Vioel,et al.  Q-switched multikilowatt CO2 laser system excited by microwaves , 1993, International Symposium on High Power Laser Systems and Applications.

[7]  Hiroki Tanaka,et al.  Emission characteristics of EUV light source by CO2 laser-produced Xe and Sn plasma , 2004, SPIE High-Power Laser Ablation.

[8]  Tatsuhiko Sakai,et al.  Q-switched CO2 laser using intense pulsed rf discharge and high-speed rotating chopper , 1995, International Symposium on High Power Laser Systems and Applications.

[9]  Hiroki Tanaka,et al.  Comparative study on emission characteristics of extreme ultraviolet radiation from CO2 and Nd:YAG laser-produced tin plasmas , 2005 .

[10]  Denis R. Hall,et al.  Power scaling of large‐area transverse radio frequency discharge CO2 lasers , 1989 .

[11]  D. R. Hall,et al.  An efficient, RF excited, waveguide CO2 laser , 1981 .

[12]  Denis R. Hall,et al.  Transverse mode propagation and gain coefficients in a planar waveguide CO/sub 2/ laser amplifier , 2001 .

[13]  Tatsuya Ariga,et al.  Development of short pulse and high power CO2 laser for EUV lithography , 2005, SPIE Optics + Photonics.