Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances

Abstract When laser beams propagate through media with non-vanishing absorption, the media is heated resulting in a change of the refractive index, which can lead to thermal lensing and thermal blooming. However, experimental details about both phenomena for propagations in water are lacking, especi...

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Autores principales: Stefan Reich, Sebastian Schäffer, Martin Lueck, Matthias Wickert, Jens Osterholz
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Lenguaje:EN
Publicado: Nature Portfolio 2021
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Acceso en línea:https://doaj.org/article/408e68532439415cb1360871d11c50fe
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spelling oai:doaj.org-article:408e68532439415cb1360871d11c50fe2021-11-21T12:18:05ZContinuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances10.1038/s41598-021-02112-62045-2322https://doaj.org/article/408e68532439415cb1360871d11c50fe2021-11-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-02112-6https://doaj.org/toc/2045-2322Abstract When laser beams propagate through media with non-vanishing absorption, the media is heated resulting in a change of the refractive index, which can lead to thermal lensing and thermal blooming. However, experimental details about both phenomena for propagations in water are lacking, especially for high-power lasers in the kilowatt range. We show that significant thermal lensing occurs only for high input powers before the onset of convective flow, while for low input powers, no strong thermal lens arises. After the onset of water flow, thermal blooming occurs at low input powers comparable to that known for propagations over kilometres in the air. However, for high input powers a thermal blooming on a qualitatively higher level is shown. By wavefront sensing, the change of refractive index distribution in water is investigated. This clearly shows the fast development of a strong thermal lens for high input powers and the onset of convection. Furthermore, a qualitatively good agreement of the accompanying simulations is observed. It is found that the absorption coefficient is linear with a value of $$\mu ={13.7}\,{\mathrm{m}^{-1}}$$ μ = 13.7 m - 1 at least up to 7.5 kW, i.e. 8  $$\mathrm{kW/cm}^2$$ kW / cm 2 . However, the directed transmission into an aperture is only constant before any thermal lensing of blooming occurs.Stefan ReichSebastian SchäfferMartin LueckMatthias WickertJens OsterholzNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-10 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Stefan Reich
Sebastian Schäffer
Martin Lueck
Matthias Wickert
Jens Osterholz
Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
description Abstract When laser beams propagate through media with non-vanishing absorption, the media is heated resulting in a change of the refractive index, which can lead to thermal lensing and thermal blooming. However, experimental details about both phenomena for propagations in water are lacking, especially for high-power lasers in the kilowatt range. We show that significant thermal lensing occurs only for high input powers before the onset of convective flow, while for low input powers, no strong thermal lens arises. After the onset of water flow, thermal blooming occurs at low input powers comparable to that known for propagations over kilometres in the air. However, for high input powers a thermal blooming on a qualitatively higher level is shown. By wavefront sensing, the change of refractive index distribution in water is investigated. This clearly shows the fast development of a strong thermal lens for high input powers and the onset of convection. Furthermore, a qualitatively good agreement of the accompanying simulations is observed. It is found that the absorption coefficient is linear with a value of $$\mu ={13.7}\,{\mathrm{m}^{-1}}$$ μ = 13.7 m - 1 at least up to 7.5 kW, i.e. 8  $$\mathrm{kW/cm}^2$$ kW / cm 2 . However, the directed transmission into an aperture is only constant before any thermal lensing of blooming occurs.
format article
author Stefan Reich
Sebastian Schäffer
Martin Lueck
Matthias Wickert
Jens Osterholz
author_facet Stefan Reich
Sebastian Schäffer
Martin Lueck
Matthias Wickert
Jens Osterholz
author_sort Stefan Reich
title Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
title_short Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
title_full Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
title_fullStr Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
title_full_unstemmed Continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
title_sort continuous wave high-power laser propagation in water is affected by strong thermal lensing and thermal blooming already at short distances
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/408e68532439415cb1360871d11c50fe
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AT martinlueck continuouswavehighpowerlaserpropagationinwaterisaffectedbystrongthermallensingandthermalbloomingalreadyatshortdistances
AT matthiaswickert continuouswavehighpowerlaserpropagationinwaterisaffectedbystrongthermallensingandthermalbloomingalreadyatshortdistances
AT jensosterholz continuouswavehighpowerlaserpropagationinwaterisaffectedbystrongthermallensingandthermalbloomingalreadyatshortdistances
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