Weir et al., 1990 - Google Patents
Increase in the flux‐pinning energy of YBa2Cu3O7− δ by shock compactionWeir et al., 1990
- Document ID
- 8597654146477163466
- Author
- Weir S
- Nellis W
- Kramer M
- Seaman C
- Early E
- Maple M
- Publication year
- Publication venue
- Applied physics letters
External Links
Snippet
FIG. 1. Zero-field-cooled diamagnetic susceptibility at 30 Oe as a function of temperature for the starting YBaOCu,, 07_ f,+ Ag powder, the asshocked YBa2Cu3 0 7 _ b+ Ag composite, and the shocked+ annealed composite. Annealing the shocked specimen does not restore …
- 230000035939 shock 0 title abstract description 21
Classifications
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/02—Details
- H01L39/12—Details characterised by the material
- H01L39/125—Ceramic materials
- H01L39/126—Ceramic materials comprising copper oxide
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/24—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof
- H01L39/2419—Processes or apparatus peculiar to the manufacture or treatment of devices provided for in H01L39/00 or of parts thereof the superconducting material comprising copper oxide
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H01L39/00—Devices using superconductivity; Processes or apparatus peculiar to the manufacture or treatment thereof or of parts thereof
- H01L39/22—Devices comprising a junction of dissimilar materials, e.g. Josephson-effect devices
- H01L39/223—Josephson-effect devices
- H01L39/225—Josephson-effect devices comprising high Tc ceramic materials
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S505/00—Superconductor technology: apparatus, material, process
- Y10S505/825—Apparatus per se, device per se, or process of making or operating same
- Y10S505/869—Power supply, regulation, or energy storage system
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/032—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
- H01F1/04—Metals or alloys
- H01F1/047—Alloys characterised by their composition
-
- H—ELECTRICITY
- H01—BASIC ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/0036—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity
- H01F1/0072—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity one dimensional, i.e. linear or dendritic nanostructures
- H01F1/0081—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties showing low dimensional magnetism, i.e. spin rearrangements due to a restriction of dimensions, e.g. showing giant magnetoresistivity one dimensional, i.e. linear or dendritic nanostructures in a non-magnetic matrix, e.g. Fe-nanowires in a nanoporous membrane
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Weir et al. | Increase in the flux‐pinning energy of YBa2Cu3O7− δ by shock compaction | |
Hardy et al. | Latent track formation induced by high energy heavy ions in superconductive copper oxides | |
Kadowaki et al. | Anomalous magnetization behavior of single crystalline Bi2Sr2CaCu2O8+ δ | |
Sato et al. | Anisotropy in a heavy fermion superconductor: UPd 2 Al 3 | |
Hu et al. | Enhancement of transport critical current densities in (Bi, Pb) 2Sr2Ca2Cu3O10/Ag tapes at 77 K following fast neutron irradiation | |
Thompson et al. | Superconductivity, intergrain, and intragrain critical current densities of materials | |
Franse et al. | Magnetic and superconducting properties of UPt3 | |
Hor et al. | High Critical Current Density in Neutron-Irradiated Bulk YBa 2 Cu 3 O 7 | |
Xiao et al. | Flux pinning and critical current density in Y Ba 2 Cu 3 O 6+ y and Eu Ba 2 Cu 3 O 6+ y superconductors | |
Kontani et al. | Magnetic, transport and thermal properties of CeCuAl3 single crystal | |
Iwasaki et al. | On narrowing of the resistive superconducting transition in applied magnetic fields and positive curvature in Hc2 (T) in the (Gd1− xPrx) Ba2Cu3O7− δ system | |
Thamizhavel et al. | Low temperature magnetic properties of CeTBi2 (T: Ni, Cu and Ag) single crystals | |
Shi et al. | A simple method for recycling GdBCO–Ag single grain bulk superconductors | |
Gonzalez-Arrabal et al. | Very high trapped fields in neutron irradiated and reinforced YBa 2 Cu 3 O 7− δ melt-textured superconductors | |
Williams et al. | Effect of heat treatment on the superconducting properties of cold-worked niobium | |
Xia et al. | Critical current density and the irreversibility line in melt textured YBa2Cu3Oy and YBa2Cu3OyAg superconductors | |
Hilscher et al. | The effect of Cu/Zn substitution in Nd1. 85Ce0. 15CuO4 on superconductivity studied by magnetic, transport and specific heat measurements and Raman spectroscopy | |
Gruss et al. | High trapped fields in melt-textured YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta | |
Feng et al. | Study on the properties of Sn‐added YBCO prepared by the powder melting process | |
EP0978885B1 (en) | Superconductor with high trapped field | |
Gavaler et al. | Properties of NbN films crystallized from the amorphous state | |
Gruss et al. | Superconducting permanent magnets from bulk YBa/sub 2/Cu/sub 3/O/sub 7-/spl delta//samples | |
Weir et al. | Magnetic and Electrical Properties of Shock Compacted High-Tc Superconductors | |
US5158930A (en) | Method of improving superconducting qualities of fabricated constructs by shock preprocessing of precursor materials | |
Weir et al. | Effects of shock-induced defects on flux pinning in YBa2Cu3O7− δ |