Theory of Copper Oxide Superconductors
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Electron—Phonon Interaction and Electron—Phonon Spectral Functions

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_13 ◽

2005 ◽

pp. 139-159

Keyword(s):

Phonon Interaction ◽

Spectral Functions ◽

Electron Phonon Interaction

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Experimental Results of High Temperature Superconducting Cuprates

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_2 ◽

2005 ◽

pp. 9-14

Keyword(s):

High Temperature ◽

Experimental Results ◽

Superconducting Cuprates ◽

High Temperature Superconducting

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Brief Review of Models of High-Temperature Superconducting Cuprates

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_3 ◽

2005 ◽

pp. 15-27

Keyword(s):

High Temperature ◽

Superconducting Cuprates ◽

High Temperature Superconducting

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Mechanism of High Temperature Superconductivity

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_14 ◽

2005 ◽

pp. 161-192

Keyword(s):

High Temperature ◽

High Temperature Superconductivity

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Cluster Models for Hole-Doped CuO6 Octahedron and CuO5 Pyramid

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_4 ◽

2005 ◽

pp. 29-35

Keyword(s):

Cluster Models

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The Kamimura—Suwa (K-S) Model: Electronic Structure of Underdoped Cuprates

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_8 ◽

2005 ◽

pp. 55-62

Keyword(s):

Electronic Structure ◽

Underdoped Cuprates ◽

S Model

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Introduction

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_1 ◽

2005 ◽

pp. 1-7

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Electronic Structure of a CuO5 Pyramid in Bi2Sr2CaCu2O8+δ

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_7 ◽

2005 ◽

pp. 51-53

Keyword(s):

Electronic Structure

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Normal State Properties of La2−xSrxCuO4

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_12 ◽

2005 ◽

pp. 121-137

Keyword(s):

Normal State ◽

Normal State Properties

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Calculated Results of a Hole-Doped CuO5 Pyramid in YBa2Cu3O7−δ

Theory of Copper Oxide Superconductors ◽

10.1007/3-540-27632-7_6 ◽

2005 ◽

pp. 43-49

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