Phenomenological study of spin-triplet ferromagnetic superconductors
Unconventional superconductivity with spin-triplet Cooper pairing is reviewed based on the quasi-phenomenological Ginzburg-Landau theory. The superconductivity, in particular, the mixed phase of coexistence of ferromagnetizm and unconventional superconductivity is triggered by the spontaneous ma...
Збережено в:
Дата: | 2005 |
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Автори: | , , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
2005
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Назва видання: | Condensed Matter Physics |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/119482 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Phenomenological study of spin-triplet ferromagnetic superconductors / D.V. Shopova, T.E. Tsvetkov, D.I. Uzunov // Condensed Matter Physics. — 2005. — Т. 8, № 1(41). — С. 181–192. — Бібліогр.: 53 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | Unconventional superconductivity with spin-triplet Cooper pairing is reviewed
based on the quasi-phenomenological Ginzburg-Landau theory. The
superconductivity, in particular, the mixed phase of coexistence of ferromagnetizm
and unconventional superconductivity is triggered by the spontaneous
magnetization. The mixed phase is stable whereas the other superconducting
phases that usually exist in unconventional superconductors
are either unstable, or, for particular values of the parameters of the theory,
some of these phases are metastable at relatively low temperatures in a
quite narrow domain of the phase diagram. The phase transitions from the
normal phase to the phase of coexistence is of first order while the phase
transition from the ferromagnetic phase to the coexistence phase can be
either of first or second order depending on the concrete substance. The
Cooper pair and crystal anisotropy are relevant to a more precise outline
of the phase diagram shape and reduce the degeneration of the ground
states of the system but they do not drastically effect the phase stability
domains and the thermodynamic properties of the respective phases. |
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