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Title: Jet formation in spallation of metal film from substrate under action of femtosecond laser pulse

Abstract

It is well known that during ablation by an ultrashort laser pulse, the main contribution to ablation of the substance is determined not by evaporation, but by the thermomechanical spallation of the substance. For identical metals and pulse parameters, the type of spallation is determined by film thickness d{sub f}. An important gauge is metal heating depth d{sub T} at the two-temperature stage, at which electron temperature is higher than ion temperature. We compare cases with d{sub f} < d{sub T} (thin film) and d{sub f} ≫ d{sub T} (bulk target). Radius R{sub L} of the spot of heating by an optical laser is the next (after d{sub f}) important geometrical parameter. The morphology of film bulging in cases where d{sub f} < d{sub T} on the substrate (blistering) changes upon a change in radius R{sub L} in the range from diffraction limit R{sub L} ∼ λ to high values of R{sub L} ≫ λ, where λ ∼ 1 μm is the wavelength of optical laser radiation. When d{sub f} < d{sub T}, R{sub L} ∼ λ, and F{sub abs} > F{sub m}, gold film deposited on the glass target acquires a cupola-shaped blister with a miniature frozen nanojet inmore » the form of a tip on the circular top of the cupola (F{sub abs} and F{sub m} are the absorbed energy and the melting threshold of the film per unit surface area of the film). A new physical mechanism leading to the formation of the nanojet is proposed.« less

Authors:
 [1];  [2];  [1]
  1. Russian Academy of Sciences, Landau Institute for Theoretical Physics (Russian Federation)
  2. Dukhov All-Russia Research Institute of Automatics (Russian Federation)
Publication Date:
OSTI Identifier:
22472439
Resource Type:
Journal Article
Resource Relation:
Journal Name: Journal of Experimental and Theoretical Physics; Journal Volume: 120; Journal Issue: 1; Other Information: Copyright (c) 2015 Pleiades Publishing, Inc.; Country of input: International Atomic Energy Agency (IAEA)
Country of Publication:
United States
Language:
English
Subject:
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; ABLATION; BLISTERS; COMPARATIVE EVALUATIONS; DIFFRACTION; ELECTRON TEMPERATURE; EVAPORATION; GLASS; GOLD; HEATING; ION TEMPERATURE; LASER RADIATION; MELTING; MORPHOLOGY; SPALLATION; SUBSTRATES; SURFACE AREA; THIN FILMS

Citation Formats

Inogamov, N. A., E-mail: nailinogamov@googlemail.com, Zhakhovskii, V. V., and Khokhlov, V. A. Jet formation in spallation of metal film from substrate under action of femtosecond laser pulse. United States: N. p., 2015. Web. doi:10.1134/S1063776115010136.
Inogamov, N. A., E-mail: nailinogamov@googlemail.com, Zhakhovskii, V. V., & Khokhlov, V. A. Jet formation in spallation of metal film from substrate under action of femtosecond laser pulse. United States. doi:10.1134/S1063776115010136.
Inogamov, N. A., E-mail: nailinogamov@googlemail.com, Zhakhovskii, V. V., and Khokhlov, V. A. Thu . "Jet formation in spallation of metal film from substrate under action of femtosecond laser pulse". United States. doi:10.1134/S1063776115010136.
@article{osti_22472439,
title = {Jet formation in spallation of metal film from substrate under action of femtosecond laser pulse},
author = {Inogamov, N. A., E-mail: nailinogamov@googlemail.com and Zhakhovskii, V. V. and Khokhlov, V. A.},
abstractNote = {It is well known that during ablation by an ultrashort laser pulse, the main contribution to ablation of the substance is determined not by evaporation, but by the thermomechanical spallation of the substance. For identical metals and pulse parameters, the type of spallation is determined by film thickness d{sub f}. An important gauge is metal heating depth d{sub T} at the two-temperature stage, at which electron temperature is higher than ion temperature. We compare cases with d{sub f} < d{sub T} (thin film) and d{sub f} ≫ d{sub T} (bulk target). Radius R{sub L} of the spot of heating by an optical laser is the next (after d{sub f}) important geometrical parameter. The morphology of film bulging in cases where d{sub f} < d{sub T} on the substrate (blistering) changes upon a change in radius R{sub L} in the range from diffraction limit R{sub L} ∼ λ to high values of R{sub L} ≫ λ, where λ ∼ 1 μm is the wavelength of optical laser radiation. When d{sub f} < d{sub T}, R{sub L} ∼ λ, and F{sub abs} > F{sub m}, gold film deposited on the glass target acquires a cupola-shaped blister with a miniature frozen nanojet in the form of a tip on the circular top of the cupola (F{sub abs} and F{sub m} are the absorbed energy and the melting threshold of the film per unit surface area of the film). A new physical mechanism leading to the formation of the nanojet is proposed.},
doi = {10.1134/S1063776115010136},
journal = {Journal of Experimental and Theoretical Physics},
number = 1,
volume = 120,
place = {United States},
year = {Thu Jan 15 00:00:00 EST 2015},
month = {Thu Jan 15 00:00:00 EST 2015}
}
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