1997
DOI: 10.1063/1.118409
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Excimer laser crystallization and doping of silicon films on plastic substrates

Abstract: We report the pulsed laser recrystallization and doping of thin film amorphous silicon deposited on oxide-coated polyester substrates. Although our heat-flow simulation of the laser recrystallization process indicates that the plastic is briefly subjected to temperatures above its softening point, we see no evidence of damage to the plastic or film delamination from the substrate. Film grain size is found to vary up to ∼0.1 μm. Electrical characteristics obtained from simple strip line resistors and thin film … Show more

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Cited by 170 publications
(72 citation statements)
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References 7 publications
(4 reference statements)
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“…16 A fraction of the incoming photon beam is absorbed through photoionization within 10 nm of the surface. Photoelectrons are ejected primarily in the direction of the electric field vector of the incoming radiation, 17 which is nearly normal to the mirror surface at LCLS. The inward directed electrons and electrons reflected by space-charge effects back to the mirror deposit their energy within 1000 nm of the mirror surface through electron impact ionization.…”
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confidence: 99%
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“…16 A fraction of the incoming photon beam is absorbed through photoionization within 10 nm of the surface. Photoelectrons are ejected primarily in the direction of the electric field vector of the incoming radiation, 17 which is nearly normal to the mirror surface at LCLS. The inward directed electrons and electrons reflected by space-charge effects back to the mirror deposit their energy within 1000 nm of the mirror surface through electron impact ionization.…”
mentioning
confidence: 99%
“…To compare the XFEL and UV cases, we have calculated temperature profiles using a Monte Carlo technique for the XFEL case 20 and a one-dimensional heat-flow model for the UV case. 17 We consider two limiting cases for the LCLS optics. For the HOMS irradiated at 8267 eV, the depth at which the temperature rise drops to 1 / e of the surface value of 37 K is 0.40 m, while for the SOMS at 827 eV, the surface temperature rise is 34 K and the depth is 0.025 m. We compare these values to the heat penetration depths for UV irradiation at the end of the laser pulse ͑when the temperature is highest͒.…”
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“…Laser annealing produces large-grain poly-Si and is compatible with lowtemperature substrates, despite raising the temperature above Si melting point. For instance, 30 ns excimer laser pulse take < 1 ms [742] for heating/cooling cycle for each pulse. Thus, having an appropriate barrier layer beneath the Si film, the molten Si cools back to room temperature before enough heat diffuses into the substrate causing damage.…”
Section: Discussionmentioning
confidence: 99%
“…Due to the very short duration and confinement of heat close to the surface, underlying device structures receive a minimal increase in the total thermal budget, while the a-Si film heats up enough to melt and re-solidify, crystallizing into polysilicon. In fact, the thermal impact is so small that ELA has been successfully performed even on a plastic substrate with 120 ˚C thermal processing limit 17 .…”
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confidence: 99%