2001
DOI: 10.1117/12.432509
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<title>Prototype laser-activated bimetallic thermal resist for microfabrication</title>

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Cited by 17 publications
(17 citation statements)
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“…Simulation suggests exposure is almost unchanged from 248 nm (Figure 2 (a)) down to 100 nm, a range that includes the proposed 157 nm exposure tools. Experimental results [1,2] showed 4 nsec pulses at 266 nm required ~7 mJ/cm 2 .When these simulations are extended from 248 nm to 13.4 nm the absorption increases 18% at the thickness 20 nm of each layer, and reflectivity becomes very small (<1%), indicating a better sensitivity. Indeed there is very little change in the 50 nm to 10 nm range.…”
Section: Quartzmentioning
confidence: 95%
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“…Simulation suggests exposure is almost unchanged from 248 nm (Figure 2 (a)) down to 100 nm, a range that includes the proposed 157 nm exposure tools. Experimental results [1,2] showed 4 nsec pulses at 266 nm required ~7 mJ/cm 2 .When these simulations are extended from 248 nm to 13.4 nm the absorption increases 18% at the thickness 20 nm of each layer, and reflectivity becomes very small (<1%), indicating a better sensitivity. Indeed there is very little change in the 50 nm to 10 nm range.…”
Section: Quartzmentioning
confidence: 95%
“…It is known that when the laser beam hits the film, reflection, transmission and absorption occur. Our Airy summation optical model [1,2] shows that for a 15/15 nm Bi/In film, 60 -70% of the laser light energy is absorbed at 514 nm wavelength, 30 -40% is reflected and less than 0.01% transmitted through the film. Most of the absorbed energy is transformed into heat and the temperature of the exposed area goes up.…”
Section: Thermal Modelingmentioning
confidence: 99%
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