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Fundamental Properties | |
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A New Condensed State | |
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Diamagnetism | |
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Absence of Low Energy Excitations | |
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Two Kinds of Superconductors | |
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Magnetic Properties of First Kind Superconductors | |
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Critical Field of a Long Cylinder | |
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Penetration Depths | |
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Magnetic Properties of a Sample of Arbitrary Shape: Intermediate State | |
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Magnetic Properties of Second Kind Superconductors | |
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Magnetization Curves of a Long Cylinder | |
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Vortex State: Microscopic Description | |
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Nonequilibrium Properties | |
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Description of the Condensed State | |
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Instability of the Normal State in the Presence of an Attractive Interaction | |
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Origin of the Attractive Interaction | |
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Ground State and Elementary Excitations | |
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Calculations at Finite Temperature | |
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The Self-Consistent Field Method | |
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The Bogolubov Equations | |
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Theorems on the Pair Potential and the Excitation Spectrum | |
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The Meissner Effect in Metals and Alloys | |
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Phenomenological Landau-Ginsburg Equations | |
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Introduction | |
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Construction of the Free Energy | |
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Equilibrium Equations | |
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The Two Characteristic Lengths | |
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Situations where /[psi]/ is Constant | |
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Situations where /[psi]/ Varies Spatially | |
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Structure of the Vortex Phase in Strong Fields (H[similar]H[subscript c2]) | |
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Microscopic Analysis of the Landau-Ginsburg Equations | |
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Linearized Self-Consistency Equation | |
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Landau-Ginsburg Equations | |
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Surface Problems in the Landau-Ginsburg Region | |
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Effects of Strong Magnetic Fields and of Magnetic Impurities | |
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Relation between Transition Temperature and Time-Reversal Properties | |
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Ergodic versus Nonergodic Behavior-- Gapless Superconductivity | |
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Dirty Superconductors in High Magnetic Fields | |
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Index | |