2007
DOI: 10.1063/1.2434987
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Estimation of optimum density and temperature for maximum efficiency of tin ions in Z discharge extreme ultraviolet sources

Abstract: Extreme ultraviolet (EUV) discharge-based lamps for EUV lithography need to generate extremely high power in the narrow spectrum band of 13.5±0.135 nm. A simplified collisional-radiative model and radiative transfer solution for an isotropic medium were utilized to investigate the wavelength-integrated light outputs in tin (Sn) plasma. Detailed calculations using the Hebrew University-Lawrence Livermore atomic code were employed for determination of necessary atomic data of the Sn4+ to Sn13+ charge states. The… Show more

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Cited by 30 publications
(12 citation statements)
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“…measured with Normarski interferometer. The electron density related to the maximum EUV emission is (2 − 3) × 10 18 cm −3 which is within the optimum density for the in-band EUV emission given by simulation result [7] .…”
Section: Laser-assisted Tin Dpp Euv Sourcesupporting
confidence: 80%
“…measured with Normarski interferometer. The electron density related to the maximum EUV emission is (2 − 3) × 10 18 cm −3 which is within the optimum density for the in-band EUV emission given by simulation result [7] .…”
Section: Laser-assisted Tin Dpp Euv Sourcesupporting
confidence: 80%
“…Because the plasma expansion processes after the maximum implosion in a LDP EUV source and after laser ablation in a LPP EUV source can both be considered as dominated by adiabatic expansion into the vacuum, and because the EUV-emitting plasmas in both sources have similar electron temperatures, 8,9 we can safely assume that particles in these two cases share similar motion-patterns during expansion. In our previous study on the characteristics of LPP, the expansion behaviors of electrons and neutrals were investigated using Stark broadening and laser induced fluorescence, respectively.…”
Section: Discussionmentioning
confidence: 99%
“…Tin fueled laser-assisted discharge plasma (LDP) proves to be a powerful light source for the generation of sufficient in-band 13.5 nm EUV emission. [4][5][6][7] LDP is also of great commercial interest because of its preferable conversion efficiency 8,9 and simplicity compared to other methods. In the LDP source, 13.5 nm EUV emission is generated from the hot and dense Z-pinch implosion plasma created by a laser triggered vacuum arc.…”
Section: Introductionmentioning
confidence: 99%
“…The ideal plasma source for emission into a 2% band centered at 13.5nm has an electron temperature between 35 and 40 electron volts (eV), and an electron density of 10 18~1 0 19 cm -3 [17].…”
Section: Introductionmentioning
confidence: 99%