Transverse magnetoresistance of the two-dimensional chiral metal

Physical Review B - Condensed Matter and Materials Physics

Volumn 59, Issue 7, 1999, Pages 4999-5002

  Chalker, J T ^a   Sondhi, S L ^b  

^a UNIVERSITY OF OXFORD   (United Kingdom)

^b PRINCETON UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 4243605722     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.4999     Document Type: Article

References (21)

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20. More generally, we obtain (Formula presented) in the diffusive regime. Due to the lack of rotational invariance of the system and its chirality in the x direction, a full specification of the linear transport of the chiral metal requires the full set of (Formula presented) which we expect to discuss in a future publication. Here we will limit ourselves to noting that there is no dc Hall conductance for the chiral metal, i.e., both (Formula presented) and (Formula presented) vanish in the transport limit in which (Formula presented) is taken to zero before (Formula presented)
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