63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $
Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoel...
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| Autor*in: |
Aleksashin, B. A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Anmerkung: |
© Pleiades Publishing, Ltd. 2010 |
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| Übergeordnetes Werk: |
Enthalten in: The physics of metals and metallography - Moscow : MAIK Nauka/Interperiodica Publ., 1996, 110(2010), 6 vom: Dez., Seite 582-587 |
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| Übergeordnetes Werk: |
volume:110 ; year:2010 ; number:6 ; month:12 ; pages:582-587 |
| Links: |
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| DOI / URN: |
10.1134/S0031918X10120094 |
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SPR020425317 |
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| 245 | 1 | 0 | |a 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
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| 520 | |a Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. | ||
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| 650 | 4 | |a magnetic susceptibility |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a shape-memory alloys |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a martensitic transformations |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a shape-memory effect |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Kondrat’ev, V. V. |4 aut | |
| 700 | 1 | |a Korolev, A. V. |4 aut | |
| 700 | 1 | |a Pushin, A. V. |4 aut | |
| 700 | 1 | |a Pushin, V. G. |4 aut | |
| 700 | 1 | |a Soloninin, A. V. |4 aut | |
| 700 | 1 | |a Tankeyev, A. P. |4 aut | |
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10.1134/S0031918X10120094 doi (DE-627)SPR020425317 (SPR)S0031918X10120094-e DE-627 ger DE-627 rakwb eng Aleksashin, B. A. verfasserin aut 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 Kondrat’ev, V. V. aut Korolev, A. V. aut Pushin, A. V. aut Pushin, V. G. aut Soloninin, A. V. aut Tankeyev, A. P. aut Enthalten in The physics of metals and metallography Moscow : MAIK Nauka/Interperiodica Publ., 1996 110(2010), 6 vom: Dez., Seite 582-587 (DE-627)35078227X (DE-600)2083437-8 1555-6190 nnns volume:110 year:2010 number:6 month:12 pages:582-587 https://dx.doi.org/10.1134/S0031918X10120094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 110 2010 6 12 582-587 |
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10.1134/S0031918X10120094 doi (DE-627)SPR020425317 (SPR)S0031918X10120094-e DE-627 ger DE-627 rakwb eng Aleksashin, B. A. verfasserin aut 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 Kondrat’ev, V. V. aut Korolev, A. V. aut Pushin, A. V. aut Pushin, V. G. aut Soloninin, A. V. aut Tankeyev, A. P. aut Enthalten in The physics of metals and metallography Moscow : MAIK Nauka/Interperiodica Publ., 1996 110(2010), 6 vom: Dez., Seite 582-587 (DE-627)35078227X (DE-600)2083437-8 1555-6190 nnns volume:110 year:2010 number:6 month:12 pages:582-587 https://dx.doi.org/10.1134/S0031918X10120094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 110 2010 6 12 582-587 |
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10.1134/S0031918X10120094 doi (DE-627)SPR020425317 (SPR)S0031918X10120094-e DE-627 ger DE-627 rakwb eng Aleksashin, B. A. verfasserin aut 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 Kondrat’ev, V. V. aut Korolev, A. V. aut Pushin, A. V. aut Pushin, V. G. aut Soloninin, A. V. aut Tankeyev, A. P. aut Enthalten in The physics of metals and metallography Moscow : MAIK Nauka/Interperiodica Publ., 1996 110(2010), 6 vom: Dez., Seite 582-587 (DE-627)35078227X (DE-600)2083437-8 1555-6190 nnns volume:110 year:2010 number:6 month:12 pages:582-587 https://dx.doi.org/10.1134/S0031918X10120094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 110 2010 6 12 582-587 |
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10.1134/S0031918X10120094 doi (DE-627)SPR020425317 (SPR)S0031918X10120094-e DE-627 ger DE-627 rakwb eng Aleksashin, B. A. verfasserin aut 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 Kondrat’ev, V. V. aut Korolev, A. V. aut Pushin, A. V. aut Pushin, V. G. aut Soloninin, A. V. aut Tankeyev, A. P. aut Enthalten in The physics of metals and metallography Moscow : MAIK Nauka/Interperiodica Publ., 1996 110(2010), 6 vom: Dez., Seite 582-587 (DE-627)35078227X (DE-600)2083437-8 1555-6190 nnns volume:110 year:2010 number:6 month:12 pages:582-587 https://dx.doi.org/10.1134/S0031918X10120094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 110 2010 6 12 582-587 |
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10.1134/S0031918X10120094 doi (DE-627)SPR020425317 (SPR)S0031918X10120094-e DE-627 ger DE-627 rakwb eng Aleksashin, B. A. verfasserin aut 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2010 Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 Kondrat’ev, V. V. aut Korolev, A. V. aut Pushin, A. V. aut Pushin, V. G. aut Soloninin, A. V. aut Tankeyev, A. P. aut Enthalten in The physics of metals and metallography Moscow : MAIK Nauka/Interperiodica Publ., 1996 110(2010), 6 vom: Dez., Seite 582-587 (DE-627)35078227X (DE-600)2083437-8 1555-6190 nnns volume:110 year:2010 number:6 month:12 pages:582-587 https://dx.doi.org/10.1134/S0031918X10120094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 110 2010 6 12 582-587 |
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Enthalten in The physics of metals and metallography 110(2010), 6 vom: Dez., Seite 582-587 volume:110 year:2010 number:6 month:12 pages:582-587 |
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Enthalten in The physics of metals and metallography 110(2010), 6 vom: Dez., Seite 582-587 volume:110 year:2010 number:6 month:12 pages:582-587 |
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Aleksashin, B. A. @@aut@@ Kondrat’ev, V. V. @@aut@@ Korolev, A. V. @@aut@@ Pushin, A. V. @@aut@@ Pushin, V. G. @@aut@@ Soloninin, A. V. @@aut@@ Tankeyev, A. P. @@aut@@ |
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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">63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2010</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">© Pleiades Publishing, Ltd. 2010</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. 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Aleksashin, B. A. |
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Aleksashin, B. A. misc nuclear magnetic resonance misc magnetic susceptibility misc shape-memory alloys misc martensitic transformations misc shape-memory effect 63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
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63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ nuclear magnetic resonance (dpeaa)DE-He213 magnetic susceptibility (dpeaa)DE-He213 shape-memory alloys (dpeaa)DE-He213 martensitic transformations (dpeaa)DE-He213 shape-memory effect (dpeaa)DE-He213 |
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63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
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(DE-627)SPR020425317 (SPR)S0031918X10120094-e |
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63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
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Aleksashin, B. A. |
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The physics of metals and metallography |
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Aleksashin, B. A. Kondrat’ev, V. V. Korolev, A. V. Pushin, A. V. Pushin, V. G. Soloninin, A. V. Tankeyev, A. P. |
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Elektronische Aufsätze |
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Aleksashin, B. A. |
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10.1134/S0031918X10120094 |
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63cu nmr spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ ti_{50} %$ ni_{25} %$ cu_{25} $ |
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63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
| abstract |
Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. © Pleiades Publishing, Ltd. 2010 |
| abstractGer |
Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. © Pleiades Publishing, Ltd. 2010 |
| abstract_unstemmed |
Abstract Methods of transmission and scanning electron microscopy and nuclear magnetic resonance (NMR) at 63Cu nuclei, as well as measurements of the static magnetic susceptibility χ(T) have been used to study a shape-memory alloy (SMA) $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $, which experiences a thermoelastic martensite transformation. The alloy was obtained from an amorphous ribbon in a bimodal nano- and submicrocrystalline state via a crystallization annealing for 1 h at 770 K with a subsequent quenching to room-temperature water. The resultant B2 austenite is characterized by a fine structure of the 63Cu NMR spectra, which is connected with the different distribution of 63Cu atoms on the second coordination shell. The evolution of the shape of the spectra with decreasing temperature reveals a structural transition B2 → B19. In addition, the 63Cu NMR spectra, just as the transmission electron microscopy, indicate the presence of phase separation in the alloy, with the precipitation of a TiCu (B11) phase. The temperature dependence of the static magnetic susceptibility χ(T) also indicates the occurrence of a structural transition and has a hysteretic nature of “stepped” type. The discovered stepped nature of the χ(T) dependence is explained by the bimodal size distribution of grains of the B2 phase due to the size effect of the martensitic transformation. © Pleiades Publishing, Ltd. 2010 |
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63Cu NMR spectra, magnetic susceptibility, and transmission electron microscopy of the rapidly quenched alloy $ Ti_{50} %$ Ni_{25} %$ Cu_{25} $ |
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Kondrat’ev, V. V. Korolev, A. V. Pushin, A. V. Pushin, V. G. Soloninin, A. V. Tankeyev, A. P. |
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Kondrat’ev, V. V. Korolev, A. V. Pushin, A. V. Pushin, V. G. Soloninin, A. V. Tankeyev, A. P. |
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| score |
7.4015017 |