Statements (32)
| Predicate | Object |
|---|---|
| gptkbp:instanceOf |
superconductor type
|
| gptkbp:alsoKnownAs |
hard superconductors
|
| gptkbp:application |
gptkb:particle_accelerators
magnetic levitation MRI magnets power cables |
| gptkbp:characterizedBy |
two critical magnetic fields
|
| gptkbp:coherenceLength |
short
|
| gptkbp:contrastsWith |
gptkb:Type_I_superconductors
|
| gptkbp:criticalField1 |
lower critical field (Hc1)
|
| gptkbp:criticalField2 |
upper critical field (Hc2)
|
| gptkbp:discoveredBy |
gptkb:Alexei_Abrikosov
|
| gptkbp:discoveredIn |
1952
|
| gptkbp:GinzburgLandauParameter |
>1/sqrt(2)
|
| https://www.w3.org/2000/01/rdf-schema#label |
Type II superconductors
|
| gptkbp:includes |
gptkb:YBCO
high-temperature superconductors niobium-titanium BSCCO niobium-tin |
| gptkbp:magneticFlux |
quantized in vortices
|
| gptkbp:meissnerEffect |
partial
|
| gptkbp:penetration |
large
|
| gptkbp:property |
allow partial penetration of magnetic field
exhibit mixed state (vortex state) form magnetic vortices remain superconducting between Hc1 and Hc2 |
| gptkbp:usedIn |
magnetic resonance imaging
superconducting magnets maglev trains |
| gptkbp:bfsParent |
gptkb:Superconductivity
|
| gptkbp:bfsLayer |
7
|