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M. Cardona, G. Güntherodt (1991)
Light Scattering in Solids VI, 68
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For recent data on Hg materials, see M
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Kivelson, in Fundamental Problems in Statistical Mechanics VIII
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Nature 382
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Molec
The change in notation is introduced to avoid confusion with the boson phase variables θc and θs
Composite order parameters also arise in models of oddfrequency pairing
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Shirane in Physical Properties of High Temperature Superconductors
Bar-Yam [67]. In one dimension, these models are governed by the same strong-coupling fixed point as the pseudospin model. However, they are physically very different from our model
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In particular, this paper shows explicitly how local stripe correlations develop below a crossover temperature in a model of frustrated phase separation
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Highly conducting one-dimensional solids
In an ordered LTT structure, the unit cell is doubled along the direction of a stripe, so one-hole per two sites corresponds technically to half-filling
When holes are doped into an antiferromagnetic insulator they form a slowly fluctuating array of “topological defects” (metallic stripes) in which the motion of the holes exhibits a self-organized quasi-one-dimensional electronic character. The accompanying lateral confinement of the intervening Mott-insulating regions induces a spin gap or pseudogap in the environment of the stripes. We present a theory of underdoped high-temperature superconductors and show that there is a local separation of spin and charge and that the mobile holes on an individual stripe acquire a spin gap via pair hopping between the stripe and its environment, i.e., via a magnetic analog of the usual superconducting proximity effect. In this way a high pairing scale without a large mass renormalization is established despite the strong Coulomb repulsion between the holes. Thus the mechanism of pairing is the generation of a spin gap in spatially confined Mott-insulating regions of the material in the proximity of the metallic stripes. At nonvanishing stripe densities, Josephson coupling between stripes produces a dimensional crossover to a state with long-range superconducting phase coherence. This picture is established by obtaining exact and well-controlled approximate solutions of a model of a one-dimensional electron gas in an active environment. An extended discussion of the experimental evidence supporting the relevance of these results to the cuprate superconductors is given.
Physical Review B – American Physical Society (APS)
Published: Sep 1, 1997
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