2011
DOI: 10.1063/1.3562143
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The effect of excitation wavelength on dynamics of laser-produced tin plasma

Abstract: We investigated the effect of the excitation wavelength on the density evolution of laser-produced tin plasmas, both experimentally and numerically. For producing plasmas, Sn targets were excited with either 10.6 lm CO 2 laser or 1.06 lm Nd:yttrium aluminum garnet laser; both are considered to be potential excitation lasers for extreme ultraviolet lithography laser-produced plasma light sources. The electron density of the plasma during the isothermal expansion regime was estimated using an interferometric tec… Show more

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Cited by 88 publications
(54 citation statements)
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“…Instead, along with collisional excitation of the plume, ambient air also affects the plasma chemistry through oxide and other reactive species formation [32]. temperature can reach > 10 eV [34,35]. According to Singh et al [36], assuming adiabatic and spherical expansion of the plume, both these parameters decay by ~ 1/r 3 with space where r is the radius of the plume.…”
Section: Resultsmentioning
confidence: 98%
“…Instead, along with collisional excitation of the plume, ambient air also affects the plasma chemistry through oxide and other reactive species formation [32]. temperature can reach > 10 eV [34,35]. According to Singh et al [36], assuming adiabatic and spherical expansion of the plume, both these parameters decay by ~ 1/r 3 with space where r is the radius of the plume.…”
Section: Resultsmentioning
confidence: 98%
“…where Z is the average charge, C; n i is the Ion number density, cm -3 ; v 0 is the incident frequency, Hz; T i is the particle temperature, K; and Assuming that one electron is excited from each atom in local thermal equilibrium, then the free electron concentration can be obtained using the Saha equation: In the duration and end phases of the laser pulses, the generated plasma motion generally can be divided into two processes: isothermal expansion and adiabatic expansion [15]. In laser ablation, only the process related to the shielding effect caused by laser adsorption (i.e., isothermal expansion) was studied.…”
Section: The Plasma Shielding Effectmentioning
confidence: 99%
“…Theoretical and experimental studies [20,[30][31][32] have shown that the~10−μm wavelength generated by CO 2 lasers is favourable for LPP EUV source over the~1−μm wave− length delivered by solid−state lasers in terms of higher CE and reduced debris production [23,24]. An optimal times− cale for an energy coupling from the laser field to the plasma, dictated by the expansion dynamics, was found to be a few nanoseconds for the Nd:YAG lasers [33] and around ten nanoseconds for the CO 2 lasers [31].…”
Section: Pulse Format Requirements For 135 Nm Lpp Euv Sourcementioning
confidence: 99%