1985
DOI: 10.1007/bf00871878
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Dynamics of nanosecond laser annealing of silicon

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Cited by 11 publications
(14 citation statements)
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“…The reason for the discrepancy between the simulation results and the experimental data was due to the fact that the solution of the Stefan problem given in Ref. [10] was obtained in the one-dimensional approximation, i.e. the phase transition front was assumed to be perfectly plane.…”
Section: Resultsmentioning
confidence: 95%
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“…The reason for the discrepancy between the simulation results and the experimental data was due to the fact that the solution of the Stefan problem given in Ref. [10] was obtained in the one-dimensional approximation, i.e. the phase transition front was assumed to be perfectly plane.…”
Section: Resultsmentioning
confidence: 95%
“…The absorption coefficient of the probe radiation was ~ 10 6 cm" 1 in the melt (regarded as a liquid metal) and the rise of R to its quasisteady maximum required formation of a molten layer of just ~20 nm thick. Simulation of this specific experimental regime [10] predicted an initial melting rate of ~20 m s~' and the final crystallisation rate of ~ 3 m s"' when the radiation energy density was 2.5 J cm" 2 . Consequently, the rise time of R should be ~ 1 ns and its decay time should be less than 10 ns.…”
Section: Resultsmentioning
confidence: 95%
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“…At the same time, the measurements results don't agree with calculated data, especially if W 2 JIcm2. The calculation has been carried out by numerical solving the Stefan problem in one-dimensional approximation [9] with taking into account the temperature dependencies of thermal and optical parameters of c-Si and 1-Si. We assume that under these conditions there is possible an additional (convective) heat transfer from the surface layer (where the laser radiation is absorbed) to the melting front.…”
Section: Resultsmentioning
confidence: 99%