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CO2 Laser and Sn Droplet Target Development for EUVL
We present the development status of the two key technologies that are the high-power RF-excited CO2 laser and the Sn droplet target developed at EUVA for a HVM LaserProduced Plasma EUV light source.
Akira Endo, Hideo Hoshino, Tatsuya Ariga, Takashi Suganuma, Masato Moriya, Takayuki Yabu, Hiroshi Someya, Yoshifumi Ueno, Masaki Nakano,Takeshi Asayama, Tamotsu Abe, Hiroshi Komori, Georg Soumagne, Hakaru Mizoguchi, Akira Sumitani and Koichi Toyoda
EUVA / Extreme Ultraviolet Lithography System Development AssociationHiratsuka Research and Development Center, 1200 Manda, Hiratsuka, 254-8567 Japan [email protected]
Abstract
This work was supported by the New Energy and Industrial TechnologyDevelopment Organization (NEDO), Japan.
Summary
• High power and short pulse RF-excited CO2 MOPAlaser performance:
ü Output Power: 6 kWü Pulse Width: 22 nsü Repetition Rate: 100 kHz
• Sn droplet supplyü High-speed droplet target demonstrated
• EUV generationü IF 40W EUV power (source power 110 W, 2pi sr, 2%bw) was
produced with 5-kW CO2 laser and Sn rotating platetarget
• Next Stepü EUV generation with high power CO2 laser and high
speed Sn droplet target
High Power Short Pulse CO2 Laser for LPP EUV Source
Block Diagram
Short Pulse (FWHM:15 ns) amplification performanceOutput power Beam quality
High Power and Sort pulse RF-excited MOPACO2 laser for LPP EUV light source High-speed droplet generator
6 kw
High Speed Sn Droplet Supply
Sn droplet: Diameter 70 um,50 mm from nozzle, positionstability sigma 8 um
IF 40W EUV power (source power 110 W, 2p sr, 2%bw)was produced from CO2 laser produced Sn plasma.
EUV power : 40 W at IF (primary source to IF 34%)110 W at primary source (2 pisr、2%bw)
Irradiation condition: Target : Rotating Sn plate Laser irradiation power: 5 kW
Conversion efficiency (CE):2.2 %EUV energy stability : 8% (3sigma, 50 pulse)
EUV Generation