Klaus Fabricius
University of Wuppertal
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Featured researches published by Klaus Fabricius.
arXiv: Statistical Mechanics | 2001
Tetsuo Deguchi; Klaus Fabricius; Barry M. McCoy
We demonstrate that the six vertex model (XXZ spin chain) with Δ=(q+q-1)/2 and q2N=1 has an invariance under the loop algebra of sl2 which produces a special set of degenerate eigenvalues. For Δ=0 we compute the multiplicity of the degeneracies using Jordan–Wigner techniques.
Journal of Statistical Physics | 2001
Klaus Fabricius; Barry M. McCoy
We demonstrate for the six vertex and XXZ model parameterized by Δ= −(q+q-1)/2≠±1 that when q2N=1 for integer N≥2 the Bethes ansatz equations determine only the eigenvectors which are the highest weights of the infinite dimensional sl2 loop algebra symmetry group of the model. Therefore in this case the Bethes ansatz equations are incomplete and further conditions need to be imposed in order to completely specify the wave function. We discuss how the evaluation parameters of the finite dimensional representations of the sl2 loop algebra can be used to complete this specification.
Journal of Statistical Physics | 2003
Klaus Fabricius; Barry M. McCoy
We demonstrate that the Q matrix introduced in Baxters 1972 solution of the eight vertex model has some eigenvectors which are not eigenvectors of the spin reflection operator and conjecture a new functional equation for Q(v) which both contains the Bethe equation that gives the eigenvalues of the transfer matrix and computes the degeneracies of these eigenvalues.
arXiv: Statistical Mechanics | 2002
Klaus Fabricius; Barry M. McCoy
We propose an expression for the current form of the lowering operator of the sl 2 loop algebra symmetry of the six-vertex model (XXZ spin chain) at roots of unity. This operator has poles which correspond to the evaluation parameters of representation theory which are given as the roots of the Drinfeld polynomial. We explicitly compute these polynomials in terms of the Bethe roots which characterize the highest weight states for all values of S z . From these polynomials we find that the Bethe roots satisfy sum rules for each value of S z .
Journal of Statistical Physics | 2000
Klaus Fabricius; Barry M. McCoy
In a previous paper we demonstrated that Bethes equations are not sufficient to specify the eigenvectors of the XXZ model at roots of unity for states where the Hamiltonian has degenerate eigenvalues. We here find the equations which will complete the specification of the eigenvectors in these degenerate cases and present evidence that the sl2 loop algebra symmetry is sufficiently powerful to determine that the highest weight of each irreducible representation is given by Bethes ansatz.
Journal of Statistical Physics | 2005
Klaus Fabricius; Barry M. McCoy
AbstractWe study the transfer matrix of the 8 vertex model with an odd number of lattice sites N. For systems at the root of unity pointsη=mK/L with m odd the transfer matrix is known to satisfy the famous ‘‘TQ’’ equation where Q(υ) is a specifically known matrix. We demonstrate that the location of the zeroes of this Q(υ) matrix is qualitatively different from the case of evenN and in particular they satisfy a previously unknown equation which is more general than what is often called ‘‘Bethe’s equation.’’ For the case of even m where no Q(υ) matrix is known we demonstrate that there are many states which are not obtained from the formalism of the SOS model but which do satisfy the TQ equation. The ground state for the particular case of η=2K/3 and N odd is investigated in detail.
Physical Review B | 1998
Klaus Fabricius; Barry M. McCoy
We study the long time behavior of the zz and xx time dependent autocorrelation function of the spin 1/2 XXZ chain at
Journal of Physics A | 2007
Klaus Fabricius
T=\infty
Journal of Physics A | 2006
Klaus Fabricius; Barry M. McCoy
by exact diagonalizations on a chain of 16 sites. We find that the numerical results for the zz correlation are very well fit by the formula
Physical Review Letters | 1999
Klaus Fabricius; Andreas Klümper; Barry M. McCoy
t^{-d}[A+Be^{-\gamma (t-t_0)}\cos \Omega(t-t_0)].