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Volumn 81, Issue 21, 2010, Pages

Generalized hard-core dimer model approach to low-energy Heisenberg frustrated antiferromagnets: General properties and application to the kagome antiferromagnet

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EID: 77955341098     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.214413     Document Type: Article
Times cited : (54)

References (57)
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    • The spectrum of the GQDM is invariant under a global change in sign of all kinetic processes around single hexagons. This corresponds to a change between bosonic and fermionic conventions for the dimers as discussed, for the square lattice, in the second paper of Ref..
    • The spectrum of the GQDM is invariant under a global change in sign of all kinetic processes around single hexagons. This corresponds to a change between bosonic and fermionic conventions for the dimers as discussed, for the square lattice, in the second paper of Ref..
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    • Note that a bosonic convention has been used in Refs. leading to an overall change in sign for all the kinetic processes in Eq..
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    • Reference also investigates numerically all higher-order resonances on a small finite 36-site cluster (restricting to the relevant topological sector)
    • Reference also investigates numerically all higher-order resonances on a small finite 36-site cluster (restricting to the relevant topological sector).
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    • For the same procedure on the frustrated quantum antiferromagnet on the square lattice see, 10.1103/PhysRevB.80.184427
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    • The GQDM defined here has no diagonal terms and equal amplitudes for all 32 kinetic processes involving loops encircling a single hexagon
    • The GQDM defined here has no diagonal terms and equal amplitudes for all 32 kinetic processes involving loops encircling a single hexagon.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.