Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system
Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se an...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Chamuah, Anil [verfasserIn] Bhattacharya, Koyel [verfasserIn] Ali, Mir Sahidul [verfasserIn] Ghosh, Chandan Kumar [verfasserIn] Chattopadhyay, Dipankar [verfasserIn] Bhattacharya, Sanjib [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2021 |
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| Schlagwörter: |
S doped chalcogenide glassy system and microstructure DC conductivity and debye temperature |
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| Anmerkung: |
© The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021 |
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| Übergeordnetes Werk: |
Enthalten in: Applied physics - Berlin : Springer, 1973, 127(2021), 9 vom: 10. Aug. |
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| Übergeordnetes Werk: |
volume:127 ; year:2021 ; number:9 ; day:10 ; month:08 |
| Links: |
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| DOI / URN: |
10.1007/s00339-021-04796-z |
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| Katalog-ID: |
SPR044777140 |
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| 520 | |a Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. | ||
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| 650 | 4 | |a DC conductivity and debye temperature |7 (dpeaa)DE-He213 | |
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10.1007/s00339-021-04796-z doi (DE-627)SPR044777140 (SPR)s00339-021-04796-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Chamuah, Anil verfasserin aut Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system 2021 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 2021 Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 Bhattacharya, Koyel verfasserin aut Ali, Mir Sahidul verfasserin aut Ghosh, Chandan Kumar verfasserin aut Chattopadhyay, Dipankar verfasserin aut Bhattacharya, Sanjib verfasserin aut Enthalten in Applied physics Berlin : Springer, 1973 127(2021), 9 vom: 10. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:127 year:2021 number:9 day:10 month:08 https://dx.doi.org/10.1007/s00339-021-04796-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 33.60 ASE 51.00 ASE 53.09 ASE AR 127 2021 9 10 08 |
| spelling |
10.1007/s00339-021-04796-z doi (DE-627)SPR044777140 (SPR)s00339-021-04796-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Chamuah, Anil verfasserin aut Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system 2021 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 2021 Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 Bhattacharya, Koyel verfasserin aut Ali, Mir Sahidul verfasserin aut Ghosh, Chandan Kumar verfasserin aut Chattopadhyay, Dipankar verfasserin aut Bhattacharya, Sanjib verfasserin aut Enthalten in Applied physics Berlin : Springer, 1973 127(2021), 9 vom: 10. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:127 year:2021 number:9 day:10 month:08 https://dx.doi.org/10.1007/s00339-021-04796-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 33.60 ASE 51.00 ASE 53.09 ASE AR 127 2021 9 10 08 |
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10.1007/s00339-021-04796-z doi (DE-627)SPR044777140 (SPR)s00339-021-04796-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Chamuah, Anil verfasserin aut Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system 2021 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 2021 Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 Bhattacharya, Koyel verfasserin aut Ali, Mir Sahidul verfasserin aut Ghosh, Chandan Kumar verfasserin aut Chattopadhyay, Dipankar verfasserin aut Bhattacharya, Sanjib verfasserin aut Enthalten in Applied physics Berlin : Springer, 1973 127(2021), 9 vom: 10. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:127 year:2021 number:9 day:10 month:08 https://dx.doi.org/10.1007/s00339-021-04796-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 33.60 ASE 51.00 ASE 53.09 ASE AR 127 2021 9 10 08 |
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10.1007/s00339-021-04796-z doi (DE-627)SPR044777140 (SPR)s00339-021-04796-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Chamuah, Anil verfasserin aut Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system 2021 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 2021 Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 Bhattacharya, Koyel verfasserin aut Ali, Mir Sahidul verfasserin aut Ghosh, Chandan Kumar verfasserin aut Chattopadhyay, Dipankar verfasserin aut Bhattacharya, Sanjib verfasserin aut Enthalten in Applied physics Berlin : Springer, 1973 127(2021), 9 vom: 10. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:127 year:2021 number:9 day:10 month:08 https://dx.doi.org/10.1007/s00339-021-04796-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 33.60 ASE 51.00 ASE 53.09 ASE AR 127 2021 9 10 08 |
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10.1007/s00339-021-04796-z doi (DE-627)SPR044777140 (SPR)s00339-021-04796-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Chamuah, Anil verfasserin aut Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system 2021 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 2021 Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 Bhattacharya, Koyel verfasserin aut Ali, Mir Sahidul verfasserin aut Ghosh, Chandan Kumar verfasserin aut Chattopadhyay, Dipankar verfasserin aut Bhattacharya, Sanjib verfasserin aut Enthalten in Applied physics Berlin : Springer, 1973 127(2021), 9 vom: 10. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:127 year:2021 number:9 day:10 month:08 https://dx.doi.org/10.1007/s00339-021-04796-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 33.60 ASE 51.00 ASE 53.09 ASE AR 127 2021 9 10 08 |
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Enthalten in Applied physics 127(2021), 9 vom: 10. Aug. volume:127 year:2021 number:9 day:10 month:08 |
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Enthalten in Applied physics 127(2021), 9 vom: 10. Aug. volume:127 year:2021 number:9 day:10 month:08 |
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Ag S doped chalcogenide glassy system and microstructure DC conductivity and debye temperature XRD FE-SEM and FT-IR Mott’s variable range hopping model Greaves’s model and density of states |
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Chamuah, Anil @@aut@@ Bhattacharya, Koyel @@aut@@ Ali, Mir Sahidul @@aut@@ Ghosh, Chandan Kumar @@aut@@ Chattopadhyay, Dipankar @@aut@@ Bhattacharya, Sanjib @@aut@@ |
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X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. 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Chamuah, Anil |
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Chamuah, Anil ddc 530 bkl 33.60 bkl 51.00 bkl 53.09 misc Ag misc S doped chalcogenide glassy system and microstructure misc DC conductivity and debye temperature misc XRD misc FE-SEM and FT-IR misc Mott’s variable range hopping model misc Greaves’s model and density of states Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system |
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530 ASE 33.60 bkl 51.00 bkl 53.09 bkl Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system Ag (dpeaa)DE-He213 S doped chalcogenide glassy system and microstructure (dpeaa)DE-He213 DC conductivity and debye temperature (dpeaa)DE-He213 XRD (dpeaa)DE-He213 FE-SEM and FT-IR (dpeaa)DE-He213 Mott’s variable range hopping model (dpeaa)DE-He213 Greaves’s model and density of states (dpeaa)DE-He213 |
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ddc 530 bkl 33.60 bkl 51.00 bkl 53.09 misc Ag misc S doped chalcogenide glassy system and microstructure misc DC conductivity and debye temperature misc XRD misc FE-SEM and FT-IR misc Mott’s variable range hopping model misc Greaves’s model and density of states |
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ddc 530 bkl 33.60 bkl 51.00 bkl 53.09 misc Ag misc S doped chalcogenide glassy system and microstructure misc DC conductivity and debye temperature misc XRD misc FE-SEM and FT-IR misc Mott’s variable range hopping model misc Greaves’s model and density of states |
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ddc 530 bkl 33.60 bkl 51.00 bkl 53.09 misc Ag misc S doped chalcogenide glassy system and microstructure misc DC conductivity and debye temperature misc XRD misc FE-SEM and FT-IR misc Mott’s variable range hopping model misc Greaves’s model and density of states |
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Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system |
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Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system |
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Chamuah, Anil |
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Chamuah, Anil Bhattacharya, Koyel Ali, Mir Sahidul Ghosh, Chandan Kumar Chattopadhyay, Dipankar Bhattacharya, Sanjib |
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density of states, dc conductivity and physical properties of $ ag_{2} $s-ge–te–se chalcogenide glassy system |
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Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system |
| abstract |
Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021 |
| abstractGer |
Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021 |
| abstract_unstemmed |
Abstract Here, development of some $ Ag_{2} $S mixed chalcogenide glassy systems has been discussed in the light of DC conductivity model and variable range hopping model. X-ray diffraction (XRD) pattern has been collected to explore microstructure of them. Various nanophases such as $ Ag_{2} $Se and $ GeSe_{2} $ have been pointed out from XRD studies. Defects have been identified in the form of dislocation, and their roles in the electrical transport properties have been established. FE-SEM micrographs exhibit their amorphous nature with distributed sharper crystal-like structure. Optical phonon frequency may cause to enhance the structural vibrations by means of increasing DC electrical conductivity. Significant enhancement of density of states near Fermi level at low and high temperatures have been explained. Present glassy structure is expected to expand to reduce the scattering cross-section for getting higher values of N($ E_{F} $) at higher temperature up to a great extent. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2021 |
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Density of states, DC conductivity and physical properties of $ Ag_{2} $S-Ge–Te–Se chalcogenide glassy system |
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| score |
7.3963633 |