Effect of nonlinearity, magnetic and nonmagnetic impurities, and spin-orbit scattering on the nonlocal microwave response of a d-wave superconductor
By using linear response theory the low-temperature microwave response of a nonlocal and nonlinear d-wave superconductor with magnetic and nonmagnetic impurities is calculated. We will show that for the local, linear, and pure sample, penetration depth, ∆λ(T), and conductivity, ∆σ1(T), vary linear...
Збережено в:
Дата: | 2016 |
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Автори: | , , |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2016
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Назва видання: | Физика низких температур |
Теми: | |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/129334 |
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Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Effect of nonlinearity, magnetic and nonmagnetic impurities, and spin-orbit scattering on the nonlocal microwave response of a d-wave superconductor / H. Yavari, M. Biderang, M. Kouhfar // Физика низких температур. — 2016. — Т. 42, № 12. — С. 1397-1405. — Бібліогр.: 41 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | By using linear response theory the low-temperature microwave response of a nonlocal and nonlinear d-wave
superconductor with magnetic and nonmagnetic impurities is calculated. We will show that for the local, linear, and
pure sample, penetration depth, ∆λ(T), and conductivity, ∆σ1(T), vary linearly with temperature, consequently the
resistance, ∆R(T), would change linearly with temperature in agreement with experimental results and for the nonlocal,
nonlinear sample the linear temperature dependences ∆R(T) change to quadratic function. For impure samples
the nonlocality and nonlinearity effects are completely hidden by impurities and the temperature dependences ∆λ(T)
and ∆σ1(T) are determined by temperature interval namely the ranges of T < T* and T* << T << Tc which T* is determined
by nonmagnetic impurity concentration and the strength of impurity scattering. For T < T*
, ∆R(T) varies as T2, on the other hand for, T* << T << Tc, ∆R(T) varies linearly with temperature. We will also show that the temperature
dependence of surface resistance is unaffected by spin-orbit interaction and magnetic impurities. |
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