2007
DOI: 10.1063/1.2735944
|View full text |Cite
|
Sign up to set email alerts
|

Optimizing 13.5nm laser-produced tin plasma emission as a function of laser wavelength

Abstract: Extreme ultraviolet lithography requires a light source at 13.5nm to match the proposed multilayer optics reflectivity. The impact of wavelength and power density on the ion distribution and electron temperature in a laser-produced plasma is calculated for Nd:YAG and CO2 lasers. A steady-state figure of merit, calculated to optimize emission as a function of laser wavelength, shows an increase with a CO2 laser. The influence of reduced electron density in the CO2 laser-produced plasma is considered in a one-di… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

2
46
0

Year Published

2010
2010
2023
2023

Publication Types

Select...
4
3

Relationship

1
6

Authors

Journals

citations
Cited by 64 publications
(48 citation statements)
references
References 30 publications
2
46
0
Order By: Relevance
“…Satellite emission at wavelengths longer than 7 nm, on the other hand, is increased using the 532-nm and 355-nm wavelengths. The decrease of the 6.7-nm emission is attributed to selfabsorption in the denser, short-wavelength plasma [17]. This behavior is supported by the dual laser irradiation experiment to control the electron density gradient, i.e., the absorption length [7,18].…”
supporting
confidence: 49%
“…Satellite emission at wavelengths longer than 7 nm, on the other hand, is increased using the 532-nm and 355-nm wavelengths. The decrease of the 6.7-nm emission is attributed to selfabsorption in the denser, short-wavelength plasma [17]. This behavior is supported by the dual laser irradiation experiment to control the electron density gradient, i.e., the absorption length [7,18].…”
supporting
confidence: 49%
“…Earlier techniques relied on focusing the laser pulse in a background gas to form a plasma shutter. [5][6][7] Plasma formation occurs at a definite time during the laser pulse and the remaining part of the pulse is Temporal profile of a TEA CO 2 laser pulse showing the two temporal components; a short intense first peak (1) followed by a second low energy long duration peak (2). The graph inset shows a close up of the first peak.…”
Section: Introductionmentioning
confidence: 99%
“…An example of a TEA CO 2 laser pulse profile is shown in Fig. 1 where the initial peak (1) and the long tail (2) are marked. The laser pulse temporal profile is problematic for two reasons.…”
Section: Introductionmentioning
confidence: 99%
See 2 more Smart Citations