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 f...
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| Veröffentlicht in: | Физика низких температур |
|---|---|
| Datum: | 2001 |
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| Format: | Artikel |
| Sprache: | Englisch |
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Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2001
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| Online Zugang: | https://nasplib.isofts.kiev.ua/handle/123456789/129001 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Zitieren: | 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. |
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Digital Library of Periodicals of National Academy of Sciences of Ukraine| _version_ | 1862737163751260160 |
|---|---|
| author | Brandt, E.H. |
| author_facet | Brandt, E.H. |
| citation_txt | 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. |
| collection | DSpace DC |
| container_title | Физика низких температур |
| description | 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.
|
| first_indexed | 2025-12-07T19:57:19Z |
| format | Article |
| fulltext | |
| id | nasplib_isofts_kiev_ua-123456789-129001 |
| institution | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| issn | 0132-6414 |
| language | English |
| last_indexed | 2025-12-07T19:57:19Z |
| publishDate | 2001 |
| publisher | Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
| record_format | dspace |
| spelling | Brandt, E.H. 2018-01-15T08:39:05Z 2018-01-15T08:39:05Z 2001 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. 0132-6414 PACS: 74.60.Ge https://nasplib.isofts.kiev.ua/handle/123456789/129001 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. en Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України Физика низких температур Статьи, посвященные столетию со дня рождения Л. В. Шубникова Geometric edge barrier in the Shubnikov phase of type II superconductors Article published earlier |
| spellingShingle | Geometric edge barrier in the Shubnikov phase of type II superconductors Brandt, E.H. Статьи, посвященные столетию со дня рождения Л. В. Шубникова |
| title | Geometric edge barrier in the Shubnikov phase of type II superconductors |
| title_full | Geometric edge barrier in the Shubnikov phase of type II superconductors |
| title_fullStr | Geometric edge barrier in the Shubnikov phase of type II superconductors |
| title_full_unstemmed | Geometric edge barrier in the Shubnikov phase of type II superconductors |
| title_short | Geometric edge barrier in the Shubnikov phase of type II superconductors |
| title_sort | geometric edge barrier in the shubnikov phase of type ii superconductors |
| topic | Статьи, посвященные столетию со дня рождения Л. В. Шубникова |
| topic_facet | Статьи, посвященные столетию со дня рождения Л. В. Шубникова |
| url | https://nasplib.isofts.kiev.ua/handle/123456789/129001 |
| work_keys_str_mv | AT brandteh geometricedgebarrierintheshubnikovphaseoftypeiisuperconductors |