High power laser heating of low absorption materials
Abstract
A model is presented and confirmed experimentally that explains the anomalous behavior observed in continuous wave (CW) excitation of thermally isolated optics. Distributed Bragg Reflector (DBR) high reflective optical thin film coatings of HfO₂ and SiO₂were prepared with a very low absorption, about 7 ppm, measured by photothermal common-path interferometry. When illuminated with a 17 kW CW laser for 30 s, the coatings survived peak irradiances of 13 MW/cm², on 500 μm diameter spot cross sections. The temperature profile of the optical surfaces was measured using a calibrated thermal imaging camera for illuminated spot sizes ranging from 500 μm to 5 mm; about the same peak temperatures were recorded regardless of spot size. This phenomenon is explained by solving the heat equation for an optic of finite dimensions and taking into account the non-idealities of the experiment. An analytical result is also derived showing the relationship between millisecond pulse to CW laser operation where (1) the heating is proportional to the laser irradiance (W/m²) for millisecond pulses, (2) the heating is proportional to the beam radius (W/m) for CW, and (3) the heating is proportional to W/m∙ tan⁻¹(√(t)/m) in the transition region between the two.
- Authors:
-
- Naval Postgraduate School, 1 University Cir, Monterey, California 93943 (United States)
- Electro Optics Center, Pennsylvania State University, 222 Northpointe Blvd., Freeport, Pennsylvania 16229 (United States)
- Publication Date:
- OSTI Identifier:
- 22305688
- Resource Type:
- Journal Article
- Journal Name:
- Journal of Applied Physics
- Additional Journal Information:
- Journal Volume: 116; Journal Issue: 12; Other Information: (c) 2014 AIP Publishing LLC; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 0021-8979
- Publisher:
- American Institute of Physics (AIP)
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; ABSORPTION; COATINGS; CROSS SECTIONS; EQUATIONS; EXCITATION; HAFNIUM OXIDES; INTERFEROMETRY; LASER RADIATION; LASER-RADIATION HEATING; OPERATION; RADIANT FLUX DENSITY; SILICON OXIDES; SURFACES; TANTALUM NITRIDES; THIN FILMS
Citation Formats
Olson, K., Talghader, J., E-mail: joey@umn.edu, Ogloza, A., and Thomas, J. High power laser heating of low absorption materials. United States: N. p., 2014.
Web. doi:10.1063/1.4896750.
Olson, K., Talghader, J., E-mail: joey@umn.edu, Ogloza, A., & Thomas, J. High power laser heating of low absorption materials. United States. https://doi.org/10.1063/1.4896750
Olson, K., Talghader, J., E-mail: joey@umn.edu, Ogloza, A., and Thomas, J. 2014.
"High power laser heating of low absorption materials". United States. https://doi.org/10.1063/1.4896750.
@article{osti_22305688,
title = {High power laser heating of low absorption materials},
author = {Olson, K. and Talghader, J., E-mail: joey@umn.edu and Ogloza, A. and Thomas, J.},
abstractNote = {A model is presented and confirmed experimentally that explains the anomalous behavior observed in continuous wave (CW) excitation of thermally isolated optics. Distributed Bragg Reflector (DBR) high reflective optical thin film coatings of HfO₂ and SiO₂were prepared with a very low absorption, about 7 ppm, measured by photothermal common-path interferometry. When illuminated with a 17 kW CW laser for 30 s, the coatings survived peak irradiances of 13 MW/cm², on 500 μm diameter spot cross sections. The temperature profile of the optical surfaces was measured using a calibrated thermal imaging camera for illuminated spot sizes ranging from 500 μm to 5 mm; about the same peak temperatures were recorded regardless of spot size. This phenomenon is explained by solving the heat equation for an optic of finite dimensions and taking into account the non-idealities of the experiment. An analytical result is also derived showing the relationship between millisecond pulse to CW laser operation where (1) the heating is proportional to the laser irradiance (W/m²) for millisecond pulses, (2) the heating is proportional to the beam radius (W/m) for CW, and (3) the heating is proportional to W/m∙ tan⁻¹(√(t)/m) in the transition region between the two.},
doi = {10.1063/1.4896750},
url = {https://www.osti.gov/biblio/22305688},
journal = {Journal of Applied Physics},
issn = {0021-8979},
number = 12,
volume = 116,
place = {United States},
year = {Sun Sep 28 00:00:00 EDT 2014},
month = {Sun Sep 28 00:00:00 EDT 2014}
}