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TECHNICAL PAPERS

Ultrafast Deformation in Femtosecond Laser Heating

[+] Author and Article Information
D. Y. Tzou

Department of Mechanical and Aerospace Engineering, University of Missouri-Columbia, Columbia, MO 65211

J. E. Beraun, J. K. Chen

Laser Effect Research Branch, Air Force Research Laboratory, Kirtland AFB, NM 87117

J. Heat Transfer 124(2), 284-292 (Sep 04, 2001) (9 pages) doi:10.1115/1.1447934 History: Received April 24, 2001; Revised September 04, 2001
Copyright © 2002 by ASME
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References

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Figures

Grahic Jump Location
Non-equilibrium electron and lattice (phonon) temperatures in the picosecond domain
Grahic Jump Location
Effect of (a) H, (b) K, (c) C, and (d) L on electron temperatures at the front (heated) surface of the thin metal film (ξ=0)
Grahic Jump Location
Compressive driving force, 2θe(∂θe/∂ξ) in Eq. (10), in gold films heated by a 100 fs laser. Same conditions as those in Fig. 1(a).
Grahic Jump Location
Straining patterns, U(ξ), developed in the thin gold film with different values of H. Same conditions as those in Fig. 1(a).
Grahic Jump Location
Maximum compressive strain at the mechanical wavefront at ξ=√Yβ. Fig. 6(b) viewing from the ξ−U plane.
Grahic Jump Location
Straining patterns, U(ξ), developed in the thin gold film with different thickness (L). Same conditions as those in Fig. 1(a).
Grahic Jump Location
Straining patterns, U(ξ), developed in the thin gold film with different values of Y. Same conditions as those in Fig. 1(a).
Grahic Jump Location
Straining patterns, U(ξ), developed in the thin gold film with a fixed surface at ξ=L in (a) 0<β<40, (b) 0<β<100, and (c) 0<β<250. Same conditions as those in Fig. 1(a).

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