Bilayer splitting in overdoped high-Tc cuprates

S. E. Barnes; S. Maekawa

doi:10.1103/PhysRevB.67.224513

Bilayer splitting in overdoped high-T_c cuprates

S. E. Barnes, S. Maekawa

Research output: Contribution to journal › Article › peer-review

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Abstract

Recent angle-resolved photoemission spectroscopy data for overdoped Bi2212 are explained. of the peak-dip-hump structure, the peak corresponds the (Formula presented) component of a hole condensate which appears at T_c. The fluctuating part of this same condensate produces the hump. The bilayer splitting is large enough to produce a bonding hole and an electron antibonding quasiparticle Fermi surface. Smaller bilayer splittings observed in some experiments reflect the interaction of the peak structure with quasiparticle states near, but not at, the Fermi surface.

Original language	English (US)
Journal	Physical Review B - Condensed Matter and Materials Physics
Volume	67
Issue number	22
DOIs	https://doi.org/10.1103/PhysRevB.67.224513
State	Published - Jun 26 2003
Externally published	Yes

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics

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10.1103/PhysRevB.67.224513

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abstract = "Recent angle-resolved photoemission spectroscopy data for overdoped Bi2212 are explained. of the peak-dip-hump structure, the peak corresponds the (Formula presented) component of a hole condensate which appears at Tc. The fluctuating part of this same condensate produces the hump. The bilayer splitting is large enough to produce a bonding hole and an electron antibonding quasiparticle Fermi surface. Smaller bilayer splittings observed in some experiments reflect the interaction of the peak structure with quasiparticle states near, but not at, the Fermi surface.",

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AB - Recent angle-resolved photoemission spectroscopy data for overdoped Bi2212 are explained. of the peak-dip-hump structure, the peak corresponds the (Formula presented) component of a hole condensate which appears at Tc. The fluctuating part of this same condensate produces the hump. The bilayer splitting is large enough to produce a bonding hole and an electron antibonding quasiparticle Fermi surface. Smaller bilayer splittings observed in some experiments reflect the interaction of the peak structure with quasiparticle states near, but not at, the Fermi surface.

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Bilayer splitting in overdoped high-T_c cuprates

Abstract

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