Bosonic model with Z3 fractionalization

Physical Review B - Condensed Matter and Materials Physics

Volumn 67, Issue 11, 2003, Pages 1151081-1151086

  Motrunich, O I ^a  

^a MASSACHUSETTS INSTITUTE OF TECHNOLOGY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; CALCULATION; ELECTRICITY; ELEMENTARY PARTICLE; FRACTIONATION; MAGNETIC FIELD; MATHEMATICAL ANALYSIS; MATHEMATICAL MODEL; PHYSICS;

EID: 0037880653     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article

References (16)

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7. O. I. Motrunich and T. Senthil, Phys. Rev. Lett. 89, 277004 (2002).
8. 2 fractionalized state is the U(1) Coulomb phase in three dimensions (Ref. 6) [see also X.-G. Wen, Phys. Rev. Lett. 88, 011 602 (2002); cond-mat/0210040 (unpublished)].
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12. T. Senthil and M. P. A. Fisher, Phys. Rev. B 62, 7850 (2000).
13. 3. We can construct such an array, e.g., by starting from a triangular lattice of the R sites, possibly with boundaries, and placing the r sites at the centers of the triangles.
14. R = 0 is indeed nontrivial.
15. E. Fradkin and S. H. Shenker, Phys. Rev. D 19, 3682 (1979).
16. † indeed acts as a raising operator on this number as suggested by the notation.