Holons on a meandering stripe: quantum numbers

dc.creatorTchernyshyov, Oleg
dc.creatorPryadko, Leonid P.
dc.date2000-01-07
dc.date2000-01-14
dc.date.accessioned2026-07-07T02:36:27Z
dc.date.available2026-07-07T02:36:27Z
dc.descriptionWe attempt to access the regime of strong coupling between charge carriers and transverse dynamics of an isolated conducting ``stripe'', such as those found in cuprate superconductors. A stripe is modeled as a partially doped domain wall in an antiferromagnet (AF), introduced in the context of two different models: the t-J model with strong Ising anisotropy, and the Hubbard model in the Hartree-Fock approximation. The domain walls with a given linear charge density are supported artificially by boundary conditions. In both models we find a regime of parameters where doped holes lose their spin and become holons (charge Q=1, spin S_z=0), which can move along the stripe without frustrating AF environment. One aspect in which the holons on the AF domain wall differ from those in an ordinary one-dimensional electron gas is their transverse degree of freedom: a mobile holon always resides on a transverse kink (or antikink) of the domain wall. This gives rise to two holon flavors and to a strong coupling between doped charges and transverse fluctuations of a stripe.
dc.descriptionMinor revisions: references updated
dc.identifierhttps://arxiv.org/abs/cond-mat/0001068
dc.identifierhttp://arxiv.org/abs/cond-mat/0001068
dc.identifierPhys. Rev. B 61, 12503 (2000)
dc.identifierdoi:10.1103/PhysRevB.61.12503
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/15925
dc.subjectStrongly Correlated Electrons
dc.titleHolons on a meandering stripe: quantum numbers
dc.typetext

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