2004
DOI: 10.1088/0022-3727/37/23/002
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Fundamentals and limits for the EUV emission of pinch plasma sources for EUV lithography

Abstract: Future extreme ultraviolet (EUV) lithography will require high radiation intensities at a wavelength around 13.5 nm. The limits of emission in this spectral range from discharge based plasmas are discussed theoretically. The discussion is based on a simple MHD approach for a xenon plasma discharge and atomic data from the ADAS software package for radiative transitions, excitation and ionization of different ionization levels. Discharge parameters are chosen for the Philips' hollow cathode triggered pinch plas… Show more

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Cited by 69 publications
(39 citation statements)
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“…The effort to improve data and modeling tools is strongly continuing. Applications are mainly in fusion (see e.g., [9]) but also in the lighting industry (see e.g., [10]) and in astrophysics [11]. It is essential for a project like ADAS to implement reliable knowledge about processes and structures of the atoms and ions of the chemical elements that occur in the plasma to be investigated.…”
Section: Introductionmentioning
confidence: 99%
“…The effort to improve data and modeling tools is strongly continuing. Applications are mainly in fusion (see e.g., [9]) but also in the lighting industry (see e.g., [10]) and in astrophysics [11]. It is essential for a project like ADAS to implement reliable knowledge about processes and structures of the atoms and ions of the chemical elements that occur in the plasma to be investigated.…”
Section: Introductionmentioning
confidence: 99%
“…An ideal variant of light source for EUV lithography is a small spherical object with enough density and an optimal temperature for the given material for EUV output. This approach is used in recent investigations [67,68] for improving EUV output efficiency, that is, the first part of this problem: possible target materials for effective radiation at the 13.5 nm area on the background of the total spectrum. However, the second part of the problem consists in the formation and efficient confinement of the EUV plasma in these optimal conditions (temperature plus enough density).…”
Section: Resultsmentioning
confidence: 99%
“…The resulting plasma is a cylindrical column with a diameter of up to 3 mm and a length of approximately 2 mm. The discharge has a duration of approximately 200 ns (typically 100-500 ns; [10]). A typical emission spectrum obtained in the EUV spectral region is shown in Figure 2.…”
Section: Experimental Set-upmentioning
confidence: 99%