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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..
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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..
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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
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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.
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