Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals

Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The a...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Rogalin, V. E. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2012

Schlagwörter:	Pore Formation Radiation Defect Optical Breakdown Breakdown Threshold Optical Damage

Übergeordnetes Werk:	Enthalten in: Bulletin of the Russian Academy of Sciences - New York, NY : Allerton Press, 2007, 76(2012), 11 vom: Nov., Seite 1205-1216
Übergeordnetes Werk:	volume:76 ; year:2012 ; number:11 ; month:11 ; pages:1205-1216

Links:	Volltext

DOI / URN:	10.3103/S1062873812110184

Katalog-ID:	SPR023162341

Internformat


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520			\|a Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated.
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650		4	\|a Radiation Defect \|7 (dpeaa)DE-He213
650		4	\|a Optical Breakdown \|7 (dpeaa)DE-He213
650		4	\|a Breakdown Threshold \|7 (dpeaa)DE-He213
650		4	\|a Optical Damage \|7 (dpeaa)DE-He213
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912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
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912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
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912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
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912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
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912			\|a GBV_ILN_2070
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936	b	k	\|a 33.00 \|q ASE
951			\|a AR
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author_variant	v e r ve ver
matchkey_str	article:19349432:2012----::fetfbobnmconooeeteootclaaeo
hierarchy_sort_str	2012
bklnumber	33.00
publishDate	2012
allfields	10.3103/S1062873812110184 doi (DE-627)SPR023162341 (SPR)S1062873812110184-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Rogalin, V. E. verfasserin aut Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated. Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213 Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 76(2012), 11 vom: Nov., Seite 1205-1216 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:76 year:2012 number:11 month:11 pages:1205-1216 https://dx.doi.org/10.3103/S1062873812110184 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_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_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 33.00 ASE AR 76 2012 11 11 1205-1216
spelling	10.3103/S1062873812110184 doi (DE-627)SPR023162341 (SPR)S1062873812110184-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Rogalin, V. E. verfasserin aut Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated. Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213 Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 76(2012), 11 vom: Nov., Seite 1205-1216 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:76 year:2012 number:11 month:11 pages:1205-1216 https://dx.doi.org/10.3103/S1062873812110184 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_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_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 33.00 ASE AR 76 2012 11 11 1205-1216
allfields_unstemmed	10.3103/S1062873812110184 doi (DE-627)SPR023162341 (SPR)S1062873812110184-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Rogalin, V. E. verfasserin aut Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated. Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213 Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 76(2012), 11 vom: Nov., Seite 1205-1216 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:76 year:2012 number:11 month:11 pages:1205-1216 https://dx.doi.org/10.3103/S1062873812110184 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_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_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 33.00 ASE AR 76 2012 11 11 1205-1216
allfieldsGer	10.3103/S1062873812110184 doi (DE-627)SPR023162341 (SPR)S1062873812110184-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Rogalin, V. E. verfasserin aut Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated. Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213 Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 76(2012), 11 vom: Nov., Seite 1205-1216 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:76 year:2012 number:11 month:11 pages:1205-1216 https://dx.doi.org/10.3103/S1062873812110184 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_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_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 33.00 ASE AR 76 2012 11 11 1205-1216
allfieldsSound	10.3103/S1062873812110184 doi (DE-627)SPR023162341 (SPR)S1062873812110184-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Rogalin, V. E. verfasserin aut Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated. Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213 Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 76(2012), 11 vom: Nov., Seite 1205-1216 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:76 year:2012 number:11 month:11 pages:1205-1216 https://dx.doi.org/10.3103/S1062873812110184 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_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_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 33.00 ASE AR 76 2012 11 11 1205-1216
language	English
source	Enthalten in Bulletin of the Russian Academy of Sciences 76(2012), 11 vom: Nov., Seite 1205-1216 volume:76 year:2012 number:11 month:11 pages:1205-1216
sourceStr	Enthalten in Bulletin of the Russian Academy of Sciences 76(2012), 11 vom: Nov., Seite 1205-1216 volume:76 year:2012 number:11 month:11 pages:1205-1216
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Pore Formation Radiation Defect Optical Breakdown Breakdown Threshold Optical Damage
dewey-raw	530
isfreeaccess_bool	false
container_title	Bulletin of the Russian Academy of Sciences
authorswithroles_txt_mv	Rogalin, V. E. @@aut@@
publishDateDaySort_date	2012-11-01T00:00:00Z
hierarchy_top_id	556723872
dewey-sort	3530
id	SPR023162341
language_de	englisch
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author	Rogalin, V. E.
spellingShingle	Rogalin, V. E. ddc 530 bkl 33.00 misc Pore Formation misc Radiation Defect misc Optical Breakdown misc Breakdown Threshold misc Optical Damage Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals
authorStr	Rogalin, V. E.
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topic_title	530 ASE 33.00 bkl Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals Pore Formation (dpeaa)DE-He213 Radiation Defect (dpeaa)DE-He213 Optical Breakdown (dpeaa)DE-He213 Breakdown Threshold (dpeaa)DE-He213 Optical Damage (dpeaa)DE-He213
topic	ddc 530 bkl 33.00 misc Pore Formation misc Radiation Defect misc Optical Breakdown misc Breakdown Threshold misc Optical Damage
topic_unstemmed	ddc 530 bkl 33.00 misc Pore Formation misc Radiation Defect misc Optical Breakdown misc Breakdown Threshold misc Optical Damage
topic_browse	ddc 530 bkl 33.00 misc Pore Formation misc Radiation Defect misc Optical Breakdown misc Breakdown Threshold misc Optical Damage
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title	Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals
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title_full	Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals
author_sort	Rogalin, V. E.
journal	Bulletin of the Russian Academy of Sciences
journalStr	Bulletin of the Russian Academy of Sciences
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title_sort	effect of absorbing microinhomogeneities on optical damage to alkali-halide crystals
title_auth	Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals
abstract	Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated.
abstractGer	Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated.
abstract_unstemmed	Abstract Micropores up to 30–100 μm in size (bulk density ∼$ 10^{5} $ $ cm^{−3} $) are obtained in NaCl, KCl, KBr, and RbI via the effect of a pulse of a $ CO_{2} $ laser with power density $ 10^{6} $–$ 10^{7} $ W $ cm^{−2} $ up to 5 μs long. When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. The annealing kinetics of micropores and the effect of the ionizing radiation on the bulk pore formation in NaCl crystals are investigated.
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title_short	Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals
url	https://dx.doi.org/10.3103/S1062873812110184
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doi_str	10.3103/S1062873812110184
up_date	2024-07-03T17:15:48.308Z
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When a pore appears, plasma formation is initiated. The average temperature is ∼5500 K and the pressure is ∼$ 10^{4} $ kg $ cm^{−2} $. The dependence of the average weight of the material removed from the pore on the energy of the crystal lattice is found. Pore formation occurs mainly via the effect of the radiation pulse, due to evaporation at the absorption wave front (velocity, 5 m $ s^{−1} $) and plastic deformation. 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Effect of absorbing microinhomogeneities on optical damage to Alkali-Halide crystals

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