Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System
Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragon...
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| Autor*in: |
Irfan Ullah, M. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2018 |
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| Schlagwörter: |
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| Anmerkung: |
© The Minerals, Metals & Materials Society 2018 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electronic materials - Warrendale, Pa : TMS, 1972, 47(2018), 4 vom: 11. Jan., Seite 2298-2305 |
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| Übergeordnetes Werk: |
volume:47 ; year:2018 ; number:4 ; day:11 ; month:01 ; pages:2298-2305 |
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| DOI / URN: |
10.1007/s11664-017-6054-z |
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| Katalog-ID: |
SPR021548730 |
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| 100 | 1 | |a Irfan Ullah, M. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
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| 520 | |a Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. | ||
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| 650 | 4 | |a dielectric properties |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a optical properties |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Hasanain, S. K. |4 aut | |
| 700 | 1 | |a Hussain, Shahzad |4 aut | |
| 700 | 1 | |a Usman, M. |4 aut | |
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10.1007/s11664-017-6054-z doi (DE-627)SPR021548730 (SPR)s11664-017-6054-z-e DE-627 ger DE-627 rakwb eng Irfan Ullah, M. verfasserin aut Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2018 Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 Hasanain, S. K. aut Hussain, Shahzad aut Usman, M. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 47(2018), 4 vom: 11. Jan., Seite 2298-2305 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:47 year:2018 number:4 day:11 month:01 pages:2298-2305 https://dx.doi.org/10.1007/s11664-017-6054-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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 47 2018 4 11 01 2298-2305 |
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10.1007/s11664-017-6054-z doi (DE-627)SPR021548730 (SPR)s11664-017-6054-z-e DE-627 ger DE-627 rakwb eng Irfan Ullah, M. verfasserin aut Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2018 Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 Hasanain, S. K. aut Hussain, Shahzad aut Usman, M. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 47(2018), 4 vom: 11. Jan., Seite 2298-2305 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:47 year:2018 number:4 day:11 month:01 pages:2298-2305 https://dx.doi.org/10.1007/s11664-017-6054-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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 47 2018 4 11 01 2298-2305 |
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10.1007/s11664-017-6054-z doi (DE-627)SPR021548730 (SPR)s11664-017-6054-z-e DE-627 ger DE-627 rakwb eng Irfan Ullah, M. verfasserin aut Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2018 Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 Hasanain, S. K. aut Hussain, Shahzad aut Usman, M. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 47(2018), 4 vom: 11. Jan., Seite 2298-2305 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:47 year:2018 number:4 day:11 month:01 pages:2298-2305 https://dx.doi.org/10.1007/s11664-017-6054-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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 47 2018 4 11 01 2298-2305 |
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10.1007/s11664-017-6054-z doi (DE-627)SPR021548730 (SPR)s11664-017-6054-z-e DE-627 ger DE-627 rakwb eng Irfan Ullah, M. verfasserin aut Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2018 Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 Hasanain, S. K. aut Hussain, Shahzad aut Usman, M. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 47(2018), 4 vom: 11. Jan., Seite 2298-2305 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:47 year:2018 number:4 day:11 month:01 pages:2298-2305 https://dx.doi.org/10.1007/s11664-017-6054-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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 47 2018 4 11 01 2298-2305 |
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10.1007/s11664-017-6054-z doi (DE-627)SPR021548730 (SPR)s11664-017-6054-z-e DE-627 ger DE-627 rakwb eng Irfan Ullah, M. verfasserin aut Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Minerals, Metals & Materials Society 2018 Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 Hasanain, S. K. aut Hussain, Shahzad aut Usman, M. aut Enthalten in Journal of electronic materials Warrendale, Pa : TMS, 1972 47(2018), 4 vom: 11. Jan., Seite 2298-2305 (DE-627)324918739 (DE-600)2032868-0 1543-186X nnns volume:47 year:2018 number:4 day:11 month:01 pages:2298-2305 https://dx.doi.org/10.1007/s11664-017-6054-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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 47 2018 4 11 01 2298-2305 |
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Irfan Ullah, M. @@aut@@ Hasanain, S. K. @@aut@@ Hussain, Shahzad @@aut@@ Usman, M. @@aut@@ |
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Irfan Ullah, M. |
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Irfan Ullah, M. misc Structural properties misc magnetic properties misc dielectric properties misc optical properties Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
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Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System Structural properties (dpeaa)DE-He213 magnetic properties (dpeaa)DE-He213 dielectric properties (dpeaa)DE-He213 optical properties (dpeaa)DE-He213 |
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Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
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(DE-627)SPR021548730 (SPR)s11664-017-6054-z-e |
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Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
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Irfan Ullah, M. |
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Irfan Ullah, M. Hasanain, S. K. Hussain, Shahzad Usman, M. |
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Elektronische Aufsätze |
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Irfan Ullah, M. |
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10.1007/s11664-017-6054-z |
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improved magnetic, dielectric and optical properties of $ pbti_{1−x} %$ fe_{x} %$ o_{3} $ (0 ≤ x ≤ 0.60) system |
| title_auth |
Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
| abstract |
Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. © The Minerals, Metals & Materials Society 2018 |
| abstractGer |
Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. © The Minerals, Metals & Materials Society 2018 |
| abstract_unstemmed |
Abstract In this study, we describe an improvement of room temperature ferromagnetism achieved in a $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) system and discuss a correlation between structural, magnetic, dielectric and optical properties. Pure $ PbTiO_{3} $ , which crystallizes in a tetragonal structure, evolved towards a cubic structure with increases in Fe content. Magnetic measurements showed that all Fe substituted samples are ferromagnetic at room temperature and maximum magnetization at 7 kOe increases with increases in Fe content. The origin and improvement of ferromagnetism is ascribed to the F-center exchange mechanism. The temperature dependence of dielectric behavior showed typical ferroelectric behavior, but ferroelectric transition temperature remained above our maximum measuring temperature. The improvement in dielectric properties of the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system may be attributed to increases of resistivity and activation energy. The decrease in band gap with increase in Fe substitution is ascribed to the decrease in c/a ratio, indicating that the optical band gap is affected by the degree of structural disorder in the $ PbFe_{x} %$ Ti_{1−x} %$ O_{3} $ system. © The Minerals, Metals & Materials Society 2018 |
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Improved Magnetic, Dielectric and Optical Properties of $ PbTi_{1−x} %$ Fe_{x} %$ O_{3} $ (0 ≤ x ≤ 0.60) System |
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https://dx.doi.org/10.1007/s11664-017-6054-z |
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Hasanain, S. K. Hussain, Shahzad Usman, M. |
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10.1007/s11664-017-6054-z |
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| score |
7.401886 |