Geometric edge barrier in the Shubnikov phase of type II superconductors
In type II superconductors the magnetic response can be irreversible due to two different reasons: vortex pinning and barriers for flux penetration. Even without bulk pinning and in absence of a microscopic Bean-Livingston surface barrier for vortex penetration, superconductors of nonell...
Збережено в:
Видавець: | Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
---|---|
Дата: | 2001 |
Автор: | |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2001
|
Назва видання: | Физика низких температур |
Теми: | |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/129001 |
Теги: |
Додати тег
Немає тегів, Будьте першим, хто поставить тег для цього запису!
|
Цитувати: | Geometric edge barrier in the Shubnikov phase of type II superconductors / E.H. Brandt // Физика низких температур. — 2001. — Т. 27, № 9-10. — С. 980-990. — Бібліогр.: 51 назв. — англ. |
Репозиторії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | In type II superconductors the magnetic response
can be irreversible due to two different reasons: vortex pinning and barriers for flux
penetration. Even without bulk pinning and in absence of a microscopic Bean-Livingston
surface barrier for vortex penetration, superconductors of nonellipsoidal shape can exhibit
a large geometric barrier for flux penetration. This edge barrier and the resulting
irreversible magnetization loops and flux-density profiles are computed from continuum
electrodynamics for superconductor strips and disks with constant thickness, both without
and with bulk pinning. Expressions are given for the field of first flux entry Hen and for
the reversibility field Hrev above which the pin-free magnetization becomes reversible.
Both fields are proportional to the lower critical field Hc1 but else depend only on the
specimen shape. These results for rectangular cross section are compared with the well
known reversible magnetic behavior of ideal ellipsoids. |
---|