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Transport in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>XX</mml:mi></mml:math>chain at zero temperature: Emergence of flat magnetization profiles

Tibor AntalInstitute for Theoretical Physics, Eötvös University, Pázmány sétány 1/a, 1117 Budapest, HungaryZoltàn RàczInstitute for Theoretical Physics, Eötvös University, Pázmány sétány 1/a, 1117 Budapest, HungaryA. RákosInstitute for Solid State Physics, Hungarian Academy of Sciences, Pf. 49, 1525 Budapest 114, HungaryGunter M. SchützInstitut für Festkörperforschung, Forschungszentrum Jülich, 52424 Jülich, Germany
1999en
ABI

Abstract

We study the connection between magnetization transport and magnetization profiles in zero-temperature XX chains. The time evolution of the transverse magnetization m(x,t) is calculated using an inhomogeneous initial state that is the ground state at fixed magnetization but with m reversed from -m(0) for x<0 to m(0) for x>0. In the long-time limit, the magnetization evolves into a scaling form m(x,t)=Phi(x/t) and the profile develops a flat part (m=Phi=0) in the (x/t)<or=c(m(0)) region. The flat region shrinks to zero if m(0)-->1/2 while it expands with the maximum velocity c(0)=1 for m(0)-->0. The states emerging in the scaling limit are compared to those of a homogeneous system where the same magnetization current is driven by a bulk field, and we find that the expectation values of various quantities (energy, occupation number in the fermionic representation) agree in the two systems.

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