On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse
Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bykovskii, N. E. [verfasserIn] Zavedeev, E. V. [verfasserIn] Senatskii, Yu. V. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Physics of the solid state - College Park, Md. : Inst., 1997, 57(2015), 4 vom: Apr., Seite 798-803 |
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| Übergeordnetes Werk: |
volume:57 ; year:2015 ; number:4 ; month:04 ; pages:798-803 |
| Links: |
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| DOI / URN: |
10.1134/S1063783415040083 |
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| Katalog-ID: |
SPR019672667 |
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| 245 | 1 | 0 | |a On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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| 520 | |a Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. | ||
| 650 | 4 | |a Acoustic Wave |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Crystal Surface |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Stimulate Raman Scattering |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Shock Wave Front |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Stimulate Brillouin Scattering |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Zavedeev, E. V. |e verfasserin |4 aut | |
| 700 | 1 | |a Senatskii, Yu. V. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Physics of the solid state |d College Park, Md. : Inst., 1997 |g 57(2015), 4 vom: Apr., Seite 798-803 |w (DE-627)269017275 |w (DE-600)1473624-X |x 1090-6460 |7 nnns |
| 773 | 1 | 8 | |g volume:57 |g year:2015 |g number:4 |g month:04 |g pages:798-803 |
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10.1134/S1063783415040083 doi (DE-627)SPR019672667 (SPR)S1063783415040083-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Bykovskii, N. E. verfasserin aut On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 Zavedeev, E. V. verfasserin aut Senatskii, Yu. V. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 57(2015), 4 vom: Apr., Seite 798-803 (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:57 year:2015 number:4 month:04 pages:798-803 https://dx.doi.org/10.1134/S1063783415040083 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.60 ASE AR 57 2015 4 04 798-803 |
| spelling |
10.1134/S1063783415040083 doi (DE-627)SPR019672667 (SPR)S1063783415040083-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Bykovskii, N. E. verfasserin aut On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 Zavedeev, E. V. verfasserin aut Senatskii, Yu. V. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 57(2015), 4 vom: Apr., Seite 798-803 (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:57 year:2015 number:4 month:04 pages:798-803 https://dx.doi.org/10.1134/S1063783415040083 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.60 ASE AR 57 2015 4 04 798-803 |
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10.1134/S1063783415040083 doi (DE-627)SPR019672667 (SPR)S1063783415040083-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Bykovskii, N. E. verfasserin aut On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 Zavedeev, E. V. verfasserin aut Senatskii, Yu. V. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 57(2015), 4 vom: Apr., Seite 798-803 (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:57 year:2015 number:4 month:04 pages:798-803 https://dx.doi.org/10.1134/S1063783415040083 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.60 ASE AR 57 2015 4 04 798-803 |
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10.1134/S1063783415040083 doi (DE-627)SPR019672667 (SPR)S1063783415040083-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Bykovskii, N. E. verfasserin aut On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 Zavedeev, E. V. verfasserin aut Senatskii, Yu. V. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 57(2015), 4 vom: Apr., Seite 798-803 (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:57 year:2015 number:4 month:04 pages:798-803 https://dx.doi.org/10.1134/S1063783415040083 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.60 ASE AR 57 2015 4 04 798-803 |
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10.1134/S1063783415040083 doi (DE-627)SPR019672667 (SPR)S1063783415040083-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Bykovskii, N. E. verfasserin aut On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 Zavedeev, E. V. verfasserin aut Senatskii, Yu. V. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 57(2015), 4 vom: Apr., Seite 798-803 (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:57 year:2015 number:4 month:04 pages:798-803 https://dx.doi.org/10.1134/S1063783415040083 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.60 ASE AR 57 2015 4 04 798-803 |
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Enthalten in Physics of the solid state 57(2015), 4 vom: Apr., Seite 798-803 volume:57 year:2015 number:4 month:04 pages:798-803 |
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Acoustic Wave Crystal Surface Stimulate Raman Scattering Shock Wave Front Stimulate Brillouin Scattering |
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Bykovskii, N. E. @@aut@@ Zavedeev, E. V. @@aut@@ Senatskii, Yu. V. @@aut@@ |
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Bykovskii, N. E. |
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Bykovskii, N. E. ddc 530 bkl 33.60 misc Acoustic Wave misc Crystal Surface misc Stimulate Raman Scattering misc Shock Wave Front misc Stimulate Brillouin Scattering On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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530 ASE 33.60 bkl On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse Acoustic Wave (dpeaa)DE-He213 Crystal Surface (dpeaa)DE-He213 Stimulate Raman Scattering (dpeaa)DE-He213 Shock Wave Front (dpeaa)DE-He213 Stimulate Brillouin Scattering (dpeaa)DE-He213 |
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ddc 530 bkl 33.60 misc Acoustic Wave misc Crystal Surface misc Stimulate Raman Scattering misc Shock Wave Front misc Stimulate Brillouin Scattering |
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ddc 530 bkl 33.60 misc Acoustic Wave misc Crystal Surface misc Stimulate Raman Scattering misc Shock Wave Front misc Stimulate Brillouin Scattering |
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On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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Bykovskii, N. E. |
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Physics of the solid state |
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Bykovskii, N. E. Zavedeev, E. V. Senatskii, Yu. V. |
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on the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
| abstract |
Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. |
| abstractGer |
Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. |
| abstract_unstemmed |
Abstract Craters on the surface of an yttrium-aluminum garnet crystal plate under irradiation by nanosecond laser pulses with an intensity of $ 10^{9} $–$ 10^{10} $ W/$ cm^{2} $ and a wide (∼500Å) spectrum have been studied. The mechanism of crater formation as a result of plastic deformation of the surface during the laser action has been discussed. The proposed mechanism takes into account specific features of nonlinear effects under the action of a broadband radiation on the medium. In the stimulated Brillouin scattering of pumping radiation, acoustic waves transform into shock waves, on the fronts of which stimulated Raman scattering develops. As a result, crystal lattice defects formed on the shock-wave fronts are dragged in the direction of pumping, which leads to a high-rate deformation of the crystal surface. |
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4 |
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On the mechanism of deformation of an yttrium-aluminum garnet crystal surface under the action of a nanosecond broadband laser pulse |
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https://dx.doi.org/10.1134/S1063783415040083 |
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Zavedeev, E. V. Senatskii, Yu. V. |
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Zavedeev, E. V. Senatskii, Yu. V. |
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2024-07-04T02:31:46.416Z |
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| score |
7.400278 |