New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K
New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The super...
Ausführliche Beschreibung
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Englisch |
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1984 |
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Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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Übergeordnetes Werk: |
in: Physica B+C - Amsterdam : Elsevier, 127(1984), 1-3, Seite 366-377 |
Übergeordnetes Werk: |
volume:127 ; year:1984 ; number:1-3 ; pages:366-377 |
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NLEJ184873231 |
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520 | |a New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. | ||
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(DE-627)NLEJ184873231 (DE-599)GBVNLZ184873231 DE-627 ger DE-627 rakwb eng New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K 1984 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Tournier, R. oth in Physica B+C Amsterdam : Elsevier 127(1984), 1-3, Seite 366-377 (DE-627)NLEJ177412429 (DE-600)2208195-1 0378-4363 nnns volume:127 year:1984 number:1-3 pages:366-377 http://dx.doi.org/10.1016/S0378-4363(84)80059-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 127 1984 1-3 366-377 |
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(DE-627)NLEJ184873231 (DE-599)GBVNLZ184873231 DE-627 ger DE-627 rakwb eng New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K 1984 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Tournier, R. oth in Physica B+C Amsterdam : Elsevier 127(1984), 1-3, Seite 366-377 (DE-627)NLEJ177412429 (DE-600)2208195-1 0378-4363 nnns volume:127 year:1984 number:1-3 pages:366-377 http://dx.doi.org/10.1016/S0378-4363(84)80059-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 127 1984 1-3 366-377 |
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(DE-627)NLEJ184873231 (DE-599)GBVNLZ184873231 DE-627 ger DE-627 rakwb eng New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K 1984 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Tournier, R. oth in Physica B+C Amsterdam : Elsevier 127(1984), 1-3, Seite 366-377 (DE-627)NLEJ177412429 (DE-600)2208195-1 0378-4363 nnns volume:127 year:1984 number:1-3 pages:366-377 http://dx.doi.org/10.1016/S0378-4363(84)80059-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 127 1984 1-3 366-377 |
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(DE-627)NLEJ184873231 (DE-599)GBVNLZ184873231 DE-627 ger DE-627 rakwb eng New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K 1984 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Tournier, R. oth in Physica B+C Amsterdam : Elsevier 127(1984), 1-3, Seite 366-377 (DE-627)NLEJ177412429 (DE-600)2208195-1 0378-4363 nnns volume:127 year:1984 number:1-3 pages:366-377 http://dx.doi.org/10.1016/S0378-4363(84)80059-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 127 1984 1-3 366-377 |
allfieldsSound |
(DE-627)NLEJ184873231 (DE-599)GBVNLZ184873231 DE-627 ger DE-627 rakwb eng New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K 1984 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Tournier, R. oth in Physica B+C Amsterdam : Elsevier 127(1984), 1-3, Seite 366-377 (DE-627)NLEJ177412429 (DE-600)2208195-1 0378-4363 nnns volume:127 year:1984 number:1-3 pages:366-377 http://dx.doi.org/10.1016/S0378-4363(84)80059-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 127 1984 1-3 366-377 |
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new experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 k |
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New experimental evidence in favor of the coexistence betweenferromagnetism and superconductivity down to 0 K |
abstract |
New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. |
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New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. |
abstract_unstemmed |
New experimental results show that the superconductivity continues to exist inside domain walls of the ferromagneticChevrel phase HoMo"6S"8. The percolation of this superconductivity can occur at very low temperatures leading to a new reentrant superconductive state below 0.15 K. The superconductivity which appears in the body-centered tetragonal phase of ErRh"4B"4 is coexisting with itinerant ferromagnetism due to the 4d electrons of Rh"4 clusters. At very low temperatures a rectangular magnetization hysteresis cycle is observed when the rare earth are ferromagnetically ordered as predicted by Tachiki for a superconductive ferromagnet. The occurrence of a p-state pairing would be the best explanation for the coexistence between the itinerant ferromagnetism and the superconductivity. |
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