The role of Replica Symmetry Breaking for localized fermionic spin
Transkript
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THE SHAPE DETERMINED BEFORE FOR THE LOCALIZED MODEL WILL BE CRUCIAL FOR THIS FILLING. THE METAL INSULATOR TRANSITION CAN NATURALLY BE EXPECTED TO OCCUR AT A CRITICAL FILLING AND A CRITICAL FINITE DENSITY OF STATES AT THE FERMI LEVEL. AS IN THE CASE OF A DISORDERED SYSTEM WITH COULOMB INTERACTION (MOTT-ANDERSON TRANSITION) THIS VALUE COULD BECOME ZERO DUE TO CRITICAL DEPLETION OF STATES, WHICH IS HOWEVER A DIMENSIONDEPENDENT EFFECT. IN THE COULOMB CASE, THE CRITICAL EXPONENT OF THE DOS-DEPLETION AT THE FERMI LEVEL DEPENDS ON SPACE DIMENSION AS FOR EXAMPLE PROPOSED IN AN (D-2)-EXPANSION (R.O., Z.Phys.B49, 273 (1983)). LOCALIZATION BY MEANS OF DISORDER CAN BE VIEWED HERE AS A CONSEQUENCE OF MAGNETIC MOMENTS WITH POSITIONAL DISORDER (but this type of disorder - in contrast to independent random potentials - is an interaction effect and the competition with quantum dynamical transport can change and suppress the moments at zero temperature in a magnetic quantum phase transition. The breakdown of magnetic order removes this particular source of localization.) fp?e q fe× mëhrgfi vt ×k j êêXçl`lëhgXèfmonbp?qrstvuw¶çÂånvmVgyxzuz{|uz}~h~h{h Ù xzuz{ |?}| Ù p?q7èfe`m,x × äæèfeYäæåtvN` Ù l}hF{h~^} Ùj ån è Yäæê *è
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