1990
DOI: 10.1051/jphys:0199000510200224300
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Analytical models of transient thermoelastic deformations of mirrors heated by high power cw laser beams

Abstract: We study the aberrations of massive mirrors heated by partial of intense laser beams in the coating or in the bulk. The non-uniform temperature field generated in the solid substrate induce thermoelastic deformations for which with the special assumption of axial symmetry, we give analytical models and numerical evaluations, first in the steady state, then in the transient regime

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Cited by 59 publications
(50 citation statements)
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(22 reference statements)
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“…The second term of u z (r) is the Saint-Venant term, in which Y is the mirror Young's modulus. The calculation of B is given by Hello and Vinet [15] 9 . This term acts to make the thermal deformation more convex.…”
Section: Summary and Discussionmentioning
confidence: 99%
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“…The second term of u z (r) is the Saint-Venant term, in which Y is the mirror Young's modulus. The calculation of B is given by Hello and Vinet [15] 9 . This term acts to make the thermal deformation more convex.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…We follow a well-known derivation by Hello and Vinet [15] and recent expansion by Vinet [27] which allows one to calculate the thermoelastic deformation induced in any axially symmetric mirror heated by absorption of an axially symmetric transmitted beam.…”
Section: Appendix a Thermoelastic Deformationmentioning
confidence: 99%
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“…The thermal variation of the material refractive index and the elastic thermal expansion at the mirror surfaces are the two dominant thermal aberrations. Hello and Vinet [13,14] predicted both the steady state and transient temperature distribution throughout a cylindrical mirror for the case where the change in temperature due to absorption of optical power remains small compared to the external ambient temperature. The time evolution of the thermal aberration per unit total absorbed power for a concentric laser beam passing through a cylindrical test mass of radius a and height h, is given by an infinite sum of exponentials as follows: are the thermo-optical coefficient, the thermal conductivity, the emissivity, and the density of the test mass material, respectively, and is the StefanBoltzmann constant.…”
mentioning
confidence: 99%
“…Figure 1 [7] shows the core optical components of an advanced interferometer, with shading showing the temperature build up in the core optical components. Thermal lensing arises whenever absorbed light in an optical substrate or coating creates a temperature gradient, which, via thermal expansion and the thermo-optic coefficient, leads to wave front distortion of the optical modes of the interferometer [9][10][11][12][13][14][15].…”
mentioning
confidence: 99%