Collective excitations in the normal state of Cu-O--based superconductors
Journal Article
·
· Phys. Rev. B: Condens. Matter; (United States)
Standard weak-coupling methods are used to calculate the excitation spectrum and the instabilities of the metallic phase of a three-band model for the copper-oxide superconductors with both intra- and intersite repulsion. Besides the magnetic excitations, a strong charge-transfer resonance of /ital A//sub 1/ital g// symmetry is predicted. For reasonable parameters, the metallic phase is found to be unstable to a charge-transfer instability at large deviations from half filling, and at small deviations to an antiferromagnet.
- Research Organization:
- ATandT Bell Laboratories, Murray Hill, New Jersey 07974(US); Serin Physics Laboratory, Rutgers University, Piscataway, New Jersey 08855
- OSTI ID:
- 5999145
- Journal Information:
- Phys. Rev. B: Condens. Matter; (United States), Journal Name: Phys. Rev. B: Condens. Matter; (United States) Vol. 39:16; ISSN PRBMD
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
36 MATERIALS SCIENCE
360204* -- Ceramics
Cermets
& Refractories-- Physical Properties
656100 -- Condensed Matter Physics-- Superconductivity
75 CONDENSED MATTER PHYSICS
SUPERCONDUCTIVITY AND SUPERFLUIDITY
CHALCOGENIDES
COLLECTIVE EXCITATIONS
COPPER COMPOUNDS
COPPER OXIDES
ENERGY-LEVEL TRANSITIONS
EXCITATION
HAMILTONIANS
INSTABILITY
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
NUCLEAR MODELS
OXIDES
OXYGEN COMPOUNDS
QUANTUM OPERATORS
SUPERCONDUCTORS
TRANSITION ELEMENT COMPOUNDS
WEAK-COUPLING MODEL
360204* -- Ceramics
Cermets
& Refractories-- Physical Properties
656100 -- Condensed Matter Physics-- Superconductivity
75 CONDENSED MATTER PHYSICS
SUPERCONDUCTIVITY AND SUPERFLUIDITY
CHALCOGENIDES
COLLECTIVE EXCITATIONS
COPPER COMPOUNDS
COPPER OXIDES
ENERGY-LEVEL TRANSITIONS
EXCITATION
HAMILTONIANS
INSTABILITY
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
NUCLEAR MODELS
OXIDES
OXYGEN COMPOUNDS
QUANTUM OPERATORS
SUPERCONDUCTORS
TRANSITION ELEMENT COMPOUNDS
WEAK-COUPLING MODEL