Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO

Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma i...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Ouis, M. A. [verfasserIn] Abd-Allah, W. M. Sallam, O. I.

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	Soda lime silicate glass UV–Vis FTIR Gamma radiation ESR

Anmerkung:	© The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022

Übergeordnetes Werk:	Enthalten in: Applied physics - Berlin : Springer, 1973, 128(2022), 5 vom: 12. Apr.
Übergeordnetes Werk:	volume:128 ; year:2022 ; number:5 ; day:12 ; month:04

Links:	Volltext

DOI / URN:	10.1007/s00339-022-05522-z

Katalog-ID:	SPR046728813

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520			\|a Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field.
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912			\|a GBV_ILN_95
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912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_267
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
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
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publishDate	2022
allfields	10.1007/s00339-022-05522-z doi (DE-627)SPR046728813 (SPR)s00339-022-05522-z-e DE-627 ger DE-627 rakwb eng Ouis, M. A. verfasserin aut Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022 Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213 Abd-Allah, W. M. aut Sallam, O. I. (orcid)0000-0001-8272-4579 aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 5 vom: 12. Apr. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:5 day:12 month:04 https://dx.doi.org/10.1007/s00339-022-05522-z 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_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_267 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_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_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_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 5 12 04
spelling	10.1007/s00339-022-05522-z doi (DE-627)SPR046728813 (SPR)s00339-022-05522-z-e DE-627 ger DE-627 rakwb eng Ouis, M. A. verfasserin aut Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022 Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213 Abd-Allah, W. M. aut Sallam, O. I. (orcid)0000-0001-8272-4579 aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 5 vom: 12. Apr. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:5 day:12 month:04 https://dx.doi.org/10.1007/s00339-022-05522-z 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_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_267 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_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_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_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 5 12 04
allfields_unstemmed	10.1007/s00339-022-05522-z doi (DE-627)SPR046728813 (SPR)s00339-022-05522-z-e DE-627 ger DE-627 rakwb eng Ouis, M. A. verfasserin aut Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022 Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213 Abd-Allah, W. M. aut Sallam, O. I. (orcid)0000-0001-8272-4579 aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 5 vom: 12. Apr. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:5 day:12 month:04 https://dx.doi.org/10.1007/s00339-022-05522-z 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_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_267 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_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_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_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 5 12 04
allfieldsGer	10.1007/s00339-022-05522-z doi (DE-627)SPR046728813 (SPR)s00339-022-05522-z-e DE-627 ger DE-627 rakwb eng Ouis, M. A. verfasserin aut Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022 Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213 Abd-Allah, W. M. aut Sallam, O. I. (orcid)0000-0001-8272-4579 aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 5 vom: 12. Apr. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:5 day:12 month:04 https://dx.doi.org/10.1007/s00339-022-05522-z 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_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_267 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_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_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_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 5 12 04
allfieldsSound	10.1007/s00339-022-05522-z doi (DE-627)SPR046728813 (SPR)s00339-022-05522-z-e DE-627 ger DE-627 rakwb eng Ouis, M. A. verfasserin aut Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022 Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213 Abd-Allah, W. M. aut Sallam, O. I. (orcid)0000-0001-8272-4579 aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 5 vom: 12. Apr. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:5 day:12 month:04 https://dx.doi.org/10.1007/s00339-022-05522-z 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_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_267 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_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_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_4126 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 5 12 04
language	English
source	Enthalten in Applied physics 128(2022), 5 vom: 12. Apr. volume:128 year:2022 number:5 day:12 month:04
sourceStr	Enthalten in Applied physics 128(2022), 5 vom: 12. Apr. volume:128 year:2022 number:5 day:12 month:04
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Soda lime silicate glass UV–Vis FTIR Gamma radiation ESR
isfreeaccess_bool	false
container_title	Applied physics
authorswithroles_txt_mv	Ouis, M. A. @@aut@@ Abd-Allah, W. M. @@aut@@ Sallam, O. I. @@aut@@
publishDateDaySort_date	2022-04-12T00:00:00Z
hierarchy_top_id	235503231
id	SPR046728813
language_de	englisch
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author	Ouis, M. A.
spellingShingle	Ouis, M. A. misc Soda lime silicate glass misc UV–Vis misc FTIR misc Gamma radiation misc ESR Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO
authorStr	Ouis, M. A.
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topic_title	Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO Soda lime silicate glass (dpeaa)DE-He213 UV–Vis (dpeaa)DE-He213 FTIR (dpeaa)DE-He213 Gamma radiation (dpeaa)DE-He213 ESR (dpeaa)DE-He213
topic	misc Soda lime silicate glass misc UV–Vis misc FTIR misc Gamma radiation misc ESR
topic_unstemmed	misc Soda lime silicate glass misc UV–Vis misc FTIR misc Gamma radiation misc ESR
topic_browse	misc Soda lime silicate glass misc UV–Vis misc FTIR misc Gamma radiation misc ESR
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO
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title_full	Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO
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author_browse	Ouis, M. A. Abd-Allah, W. M. Sallam, O. I.
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author-letter	Ouis, M. A.
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title_sort	gamma ray interaction with soda lime silicate glasses doped with $ v_{2} %$ o_{5} $, cuo or sro
title_auth	Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO
abstract	Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022
abstractGer	Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022
abstract_unstemmed	Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. New applicable trends for soda lime silicate glasses have been suggested in the radiation field. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022
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title_short	Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO
url	https://dx.doi.org/10.1007/s00339-022-05522-z
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up_date	2024-07-04T00:06:54.298Z
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A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Soda lime silicate glasses doped with one of these metal oxides: vanadium oxide, copper oxide, or strontium oxide were synthesized by high-temperature melting technique. Spectroscopic, physical and optical properties were investigated for glass samples with and without the effect of gamma irradiation at doses of 25 and 50 kGy. Absorption spectra of FTIR analysis for the samples show characteristic bands for main silicate units. In addition, FTIR analysis illustrated the stability of the glass network after gamma irradiation. The UV–Vis spectra showed absorption bands characteristic of different metal oxides in their various oxidation states in accordance with the host glass studied. Silicate groups have been found to prefer $ V^{5+} $ that appears at 245 and 335 nm. While in the case of copper doping, a peak at 313 nm is observed for $ Cu^{+} $ beside a broad peak extending from 600 to 900 nm for $ Cu^{2+} $. New defects for silicate groups at 227 and 280 nm have been appeared by adding SrO. After gamma irradiation, new defects have been observed besides some changes in the doping valences. Deconvolution of FTIR and UV spectra has been illustrated to define the overlapped peaks. Defect centers induced by ionizing gamma irradiation of glass samples have been elucidated by ESR spectroscopy. The spectrum reveals $ V^{4+} $ and $ V^{3+} $ hyperfine structures, which are well resolved. Nevertheless, the ESR spectrum shows an asymmetric line shape characteristic of a tetragonally elongated octahedral site with copper oxide-doped glass. 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Gamma ray interaction with soda lime silicate glasses doped with $ V_{2} %$ O_{5} $, CuO or SrO

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