1998/09/04 by A. Fledderjohann, Fledderjohann, A., M. Karbach +3
Physics and Astronomy · #FOS: Physical sciences #Strongly Correlated Electrons (cond-mat.str-el) #cond-mat.str-el
paper · pdf · doi:10.48550/arxiv.cond-mat/9809086
7 pages, 6 figures, LaTeX-class svjour from Springer; to be published in Eur. Phys. J. B
arxiv created 1998/09/04 · arxiv updated 2009/11/30
We study the one-dimensional spin-1/2 antiferromagnetic Heisenberg model exposed to an external field, which is a superposition of a homogeneous field h3 and a small periodic field of strength h1. For the case of a transverse staggered field a gap opens, which scales with h1^ε1, where ε1=ε1(h3) is given by the critical exponent η1(M(h3)) defined through the transverse structure factor of the model at h1=0. For the case of a longitudinal periodic field with wave vector q=π/2 and strength hq a plateau is found in the magnetization curve at M=1/4. The difference of the upper- and lower magnetic field scales with h3u-h3l∼ hq^ε3, where ε3=ε3(h3) is given by the critical exponent η3(M(h3)) defined through the longitudinal structure factor of the model at hq=0.