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Laser pulse shape dependence of poly-Si crystallization. / Prudnikov, Oleg N.; Shin, Sung Tae; Cheong, Byoung Ho.

In: AIP Advances, Vol. 7, No. 12, 125102, 01.12.2017.

Research output: Contribution to journalArticlepeer-review

Harvard

Prudnikov, ON, Shin, ST & Cheong, BH 2017, 'Laser pulse shape dependence of poly-Si crystallization', AIP Advances, vol. 7, no. 12, 125102. https://doi.org/10.1063/1.4998221

APA

Prudnikov, O. N., Shin, S. T., & Cheong, B. H. (2017). Laser pulse shape dependence of poly-Si crystallization. AIP Advances, 7(12), [125102]. https://doi.org/10.1063/1.4998221

Vancouver

Prudnikov ON, Shin ST, Cheong BH. Laser pulse shape dependence of poly-Si crystallization. AIP Advances. 2017 Dec 1;7(12):125102. doi: 10.1063/1.4998221

Author

Prudnikov, Oleg N. ; Shin, Sung Tae ; Cheong, Byoung Ho. / Laser pulse shape dependence of poly-Si crystallization. In: AIP Advances. 2017 ; Vol. 7, No. 12.

BibTeX

@article{3a91c8781ac948f79e166da47227d90e,
title = "Laser pulse shape dependence of poly-Si crystallization",
abstract = "Poly-Si crystallization mechanism is examined by conducting numerical simulations, combining the thermal diffusion equation with a rigorous coupled wave analysis method. The ripples at the boundary of poly-Si grains are modeled as a grating surface structure. Under laser beam irradiation, the melting front profiles are accurately analyzed by including surface diffraction, polarization of the laser, and laser energy density. For two different lasers, XeCl excimer laser (λ = 308 nm) and Yb:YAG solid state laser (λ= 343 nm), the energy density range at which poly-Si grains are gradually ordered was determined. Furthermore, the energy density window of the Yb:YAG laser is found to be four times larger than that of XeCl laser. On the other hand, the Yb:YAG laser may produce amorphous-Si phase after completing the crystallization process. It is suggested that this amorphous-Si phase could be avoided, if a double pulse laser is used.",
keywords = "THIN-FILM TRANSISTORS, AMORPHOUS-SILICON",
author = "Prudnikov, {Oleg N.} and Shin, {Sung Tae} and Cheong, {Byoung Ho}",
year = "2017",
month = dec,
day = "1",
doi = "10.1063/1.4998221",
language = "English",
volume = "7",
journal = "AIP Advances",
issn = "2158-3226",
publisher = "AMER INST PHYSICS",
number = "12",

}

RIS

TY - JOUR

T1 - Laser pulse shape dependence of poly-Si crystallization

AU - Prudnikov, Oleg N.

AU - Shin, Sung Tae

AU - Cheong, Byoung Ho

PY - 2017/12/1

Y1 - 2017/12/1

N2 - Poly-Si crystallization mechanism is examined by conducting numerical simulations, combining the thermal diffusion equation with a rigorous coupled wave analysis method. The ripples at the boundary of poly-Si grains are modeled as a grating surface structure. Under laser beam irradiation, the melting front profiles are accurately analyzed by including surface diffraction, polarization of the laser, and laser energy density. For two different lasers, XeCl excimer laser (λ = 308 nm) and Yb:YAG solid state laser (λ= 343 nm), the energy density range at which poly-Si grains are gradually ordered was determined. Furthermore, the energy density window of the Yb:YAG laser is found to be four times larger than that of XeCl laser. On the other hand, the Yb:YAG laser may produce amorphous-Si phase after completing the crystallization process. It is suggested that this amorphous-Si phase could be avoided, if a double pulse laser is used.

AB - Poly-Si crystallization mechanism is examined by conducting numerical simulations, combining the thermal diffusion equation with a rigorous coupled wave analysis method. The ripples at the boundary of poly-Si grains are modeled as a grating surface structure. Under laser beam irradiation, the melting front profiles are accurately analyzed by including surface diffraction, polarization of the laser, and laser energy density. For two different lasers, XeCl excimer laser (λ = 308 nm) and Yb:YAG solid state laser (λ= 343 nm), the energy density range at which poly-Si grains are gradually ordered was determined. Furthermore, the energy density window of the Yb:YAG laser is found to be four times larger than that of XeCl laser. On the other hand, the Yb:YAG laser may produce amorphous-Si phase after completing the crystallization process. It is suggested that this amorphous-Si phase could be avoided, if a double pulse laser is used.

KW - THIN-FILM TRANSISTORS

KW - AMORPHOUS-SILICON

UR - http://www.scopus.com/inward/record.url?scp=85037681948&partnerID=8YFLogxK

U2 - 10.1063/1.4998221

DO - 10.1063/1.4998221

M3 - Article

AN - SCOPUS:85037681948

VL - 7

JO - AIP Advances

JF - AIP Advances

SN - 2158-3226

IS - 12

M1 - 125102

ER -

ID: 9032235