434 research outputs found

    Second Virial Coefficient for Noncommutative Space

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    The second virial coefficient B2nc(T)B_{2}^{nc}(T) for non-interacting particles moving in a two-dimensional noncommutative space and in the presence of a uniform magnetic field B⃗\vec B is presented. The noncommutativity parameter \te can be chosen such that the B2nc(T)B_{2}^{nc}(T) can be interpreted as the second virial coefficient for anyons of statistics \al in the presence of B⃗\vec B and living on the commuting plane. In particular in the high temperature limit \be\lga 0, we establish a relation between the parameter \te and the statistics \al. Moreover, B2nc(T)B_{2}^{nc}(T) can also be interpreted in terms of composite fermions.Comment: 11 pages, misprints corrected and references adde

    Feynman path-integral approach to the QED3 theory of the pseudogap

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    In this work the connection between vortex condensation in a d-wave superconductor and the QED3_3 gauge theory of the pseudogap is elucidated. The approach taken circumvents the use of the standard Franz-Tesanovic gauge transformation, borrowing ideas from the path-integral analysis of the Aharonov-Bohm problem. An essential feature of this approach is that gauge-transformations which are prohibited on a particular multiply-connected manifold (e.g. a superconductor with vortices) can be successfully performed on the universal covering space associated with that manifold.Comment: 15 pages, 1 Figure. Int. J. Mod. Phys. B 17, 4509 (2003). Minor changes from previous versio

    Antiferromagnetism and phase separation in the t-J model at low doping: a variational study

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    Using Gutzwiller-projected wave functions, I estimate the ground-state energy of the t-J model for several variational states relevant for high-temperature cuprate superconductors. The results indicate antiferromagnetism and phase separation at low doping both in the superconducting state and in the staggered-flux normal state proposed for the vortex cores. While phase separation in the underdoped superconducting state may be relevant for the stripe formation mechanism, the results for the normal state suggest that similar charge inhomogeneities may also appear in vortex cores up to relatively high doping values.Comment: 4 pages, 3 figures, reference adde

    Non-local order in gapless systems: Entanglement Spectrum in Spin Chains

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    We show that the entanglement spectrum can be used to define non-local order in gapless spin systems. We find a gap that fully separates a series of generic, high `entanglement energy' levels, from a flat band of levels with specific multiplicities that uniquely define the ground-state, and remains finite in the thermodynamic limit. We pick the appropriate set of quantum numbers, and then partition the system in this space. This partition corresponds to a very non-local real-space cut. Despite the fact that the Laughlin state is bulk gapped while the antiferromagnetic spin chain state is bulk gapless, we show that the S=1/2 Heisenberg antiferromagnet in one dimension has an entanglement spectrum almost identical to that of the Laughlin Fractional Quantum Hall state in two dimensions, revealing the similar field theory of their low-energy edge and bulk excitations respectively.Comment: 4.5 pages, 3 figures; submitted to PRL on 10/08/09; revised version plus supplementary materia

    Critical Exponents in a Quantum Phase Transition of an Anisotropic 2D Antiferromagnet

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    I use the two-step density-matrix renormalization group method to extract the critical exponents β\beta and ν\nu in the transition from a N\'eel Q=(π,π)Q=(\pi,\pi) phase to a magnetically disordered phase with a spin gap. I find that the exponent β\beta computed from the magnetic side of the transition is consistent with that of the classical Heisenberg model, but not the exponent zνz\nu computed from the disordered side. I also show the contrast between integer and half-integer spin cases.Comment: 4 pages, 2 figure

    Free Relativistic Anyons with Canonical Spin Algebra

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    We discuss a relativistic free particle with fractional spin in 2+1 dimensions, where the dual spin components satisfy the canonical angular momentum algebra {Sμ,Sν} = ϵμνγSγ\left\{ S_\mu , S_\nu \right\}\,=\,\epsilon_{\mu \nu \gamma}S^\gamma . It is shown that it is a general consequence of these features that the Poincar\`e invariance is broken down to the Lorentz one, so indicating that it is not possible to keep simultaneously the free nature of the anyon and the translational invariance.Comment: Complete version with reference

    New Fermionic Description of Quantum S = 1/2 Antiferromargnet

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    A novel approach to S =1/2 antiferromagnets with strong fluctuations based on the representation of spin-1/2 operators as bylinear forms of real (Majorana) fermions is suggested. This representation has the advantage of being irreducible without any constraints on the fermionic Hilbert space. This property allows to derive an effective Hamiltonian for low-lying excitations in the spin liquid state. It is proven that these excitations are S = 1 real fermions.Comment: 4 page

    Scenario for Fractional Quantum Hall Effect in Bulk Isotropic Materials

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    We investigate the possibility of a strongly correlated Fractional Quantum Hall (FQH) state in bulk three dimensional isotropic (not layered) materials. We find that a FQH state can exist at low densities only if it is accompanied by a staging transition in which the electrons re-organize themselves in layers, perpendicular to the magnetic field, at distances of order the magnetic length apart. The Hartree energy associated to the staging transition is off-set by the correlation Fock energy of the 3D FQH state. We obtain the phase diagram of bulk electrons in a magnetic field subject to Coulomb interactions as a function of carrier density and lattice constant. At very low densities, the 3D FQH state exhibits a transition to a 3D Wigner crystal state stabilized by phonon correlations

    Comment on "Statistical Mechanics of Non-Abelian Chern-Simons Particles"

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    The second virial coefficient for non-Abelian Chern-Simons particles is recalculated. It is shown that the result is periodic in the flux parameter just as in the Abelian theory.Comment: 3 pages, latex fil
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