TY - JOUR
T1 - Spatial profiles of electron density, electron temperature, average ionic charge, and EUV emission of laser-produced Sn plasmas for EUV lithography
AU - Sato, Yuta
AU - Tomita, Kentaro
AU - Tsukiyama, Syoichi
AU - Eguchi, Toshiaki
AU - Uchino, Kiichiro
AU - Kouge, Kouichiro
AU - Tomuro, Hiroaki
AU - Yanagida, Tatsuya
AU - Wada, Yasunori
AU - Kunishima, Masahito
AU - Kodama, Takeshi
AU - Mizoguchi, Hakaru
N1 - Publisher Copyright:
© 2017 The Japan Society of Applied Physics.
PY - 2017/3
Y1 - 2017/3
N2 - Spatial profiles of the electron density (ne), electron temperature (Te), and average ionic charge (Z) of laser-produced Sn plasmas for EUV lithography, whose conversion efficiency (CE) is sufficiently high for practical use, were measured using a collective Thomson scattering (TS) technique. For plasma production, Sn droplets of 26μm diameter were used as a fuel. First, a picosecond-pulsed laser was used to expand a Sn target. Next, a CO2 laser was used to generate plasmas. By changing the injection timing of the picosecond and CO2 lasers, three different types of plasmas were generated. The CEs of the three types of plasmas differed, and ranged from 2.8 to 4.0%. Regarding the different plasma conditions, the spatial profiles of ne, Te, and Z clearly differed. However, under all plasma conditions, intense EUV was only observed at a sufficiently high Te (> 25 eV) and in an adequate ne range [1024-(2 × 1025)m-3]. These plasma parameters lie in the efficient-EUV light source range, as predicted by simulations.
AB - Spatial profiles of the electron density (ne), electron temperature (Te), and average ionic charge (Z) of laser-produced Sn plasmas for EUV lithography, whose conversion efficiency (CE) is sufficiently high for practical use, were measured using a collective Thomson scattering (TS) technique. For plasma production, Sn droplets of 26μm diameter were used as a fuel. First, a picosecond-pulsed laser was used to expand a Sn target. Next, a CO2 laser was used to generate plasmas. By changing the injection timing of the picosecond and CO2 lasers, three different types of plasmas were generated. The CEs of the three types of plasmas differed, and ranged from 2.8 to 4.0%. Regarding the different plasma conditions, the spatial profiles of ne, Te, and Z clearly differed. However, under all plasma conditions, intense EUV was only observed at a sufficiently high Te (> 25 eV) and in an adequate ne range [1024-(2 × 1025)m-3]. These plasma parameters lie in the efficient-EUV light source range, as predicted by simulations.
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U2 - 10.7567/JJAP.56.036201
DO - 10.7567/JJAP.56.036201
M3 - Article
AN - SCOPUS:85014383080
SN - 0021-4922
VL - 56
JO - Japanese journal of applied physics
JF - Japanese journal of applied physics
IS - 3
M1 - 036201
ER -