Two-stage model and simulation of ultra-short pulsed laser interaction with phase-change-films followed by ultra-fast cooling

A A. A. Nevzorov (Laboratory of Photonic Gas Sensors, University of Science and Technology MISIS 1 , 4 Leninsky Prospekt, Moscow 119049,) A A. A. Lotin (Mendeleev University of Chemical Technology 2 Rectorate, , 9 Miusskaya sq., Moscow 125047,) V V. A. Mikhalevsky (Petrovsky National Research Center for Surgery 4 , 2 Abrikosovsky Pereulok, Moscow 119435,) A Alexander V. Kolobov (Institute of Physics, Herzen State Pedagogical University of Russia 3 , 48 Moika Emb., St. Petersburg 191186,) O Oleg A. Louchev (Institute of Physics, Herzen State Pedagogical University of Russia 3 , 48 Moika Emb., St. Petersburg 191186,)

Abstract

In this work, we develop a computational model for ultra-short laser–matter interaction performing detailed simulations of fs pulsed 800 nm laser heating of amorphous Ge2Sb2Te5 (αGST) films, which are at the heart of re-writable optical disks and the latest generation of non-volatile electronic memory. The developed model shows good agreement with related experimental data revealing various effects of ultra-fast dynamics of the electronic subsystem photoexcitation followed by relaxation, ultra-fast cooling, re-amorphization, and partial crystallization. First, our simulations show that additional generation of free electrons by impact ionization leads to a significant decrease of the effective absorption coefficient combined with a significant temperature decrease at the film surface and a simultaneous temperature increase inside the film. Second, our simulations demonstrate the nonlinear dynamics of the dielectric function and related optical parameters. Third, our computations of the post-relaxation ultra-fast cooling dynamics combined with the equations of Arrhenius-type kinetics for crystallization elucidate the thermally controlled mechanism for the experimentally observed generation of the amorphous-crystalline-amorphous nanostructure inside the bulk of the αGST film irradiated by a fs pulsed laser. Additionally, the generation of this nanostructure is associated with an order of magnitude difference between the attempt rates involved in phase transitions (i) in the near-surface melted part and (ii) in the bulk non-melted part of the film. Finally, our study shows that a single fs pulsed laser-induced melting does not lead to the crystallization on the surface of irradiated amorphous and crystalline GST films due to onset of post-relaxation high-rate cooling 1011–1012 K/s.

Article Details

Volume / Issue Vol. 139, Issue 6
Published February 14, 2026
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (5)

A

A. A. Nevzorov

Laboratory of Photonic Gas Sensors, University of Science and Technology MISIS 1 , 4 Leninsky Prospekt, Moscow 119049,

A

A. A. Lotin

Mendeleev University of Chemical Technology 2 Rectorate, , 9 Miusskaya sq., Moscow 125047,

V

V. A. Mikhalevsky

Petrovsky National Research Center for Surgery 4 , 2 Abrikosovsky Pereulok, Moscow 119435,

A

Alexander V. Kolobov

Institute of Physics, Herzen State Pedagogical University of Russia 3 , 48 Moika Emb., St. Petersburg 191186,

O

Oleg A. Louchev

Institute of Physics, Herzen State Pedagogical University of Russia 3 , 48 Moika Emb., St. Petersburg 191186,