Even-odd effects in the SU() Heisenberg spin chain
arXiv:2302.14090 · doi:10.1103/PhysRevB.107.205135
Abstract
The zero-temperature phase diagram of the SU() antiferromagnetic Heisenberg spin chain is investigated by means of complementary field theory and numerical approaches for general . A fully gapped SU() valence bond solid made of sites is formed above a critical value of for all . We find that the extension of this -merized phase for larger values of strongly depends on the parity of . For even , the phase smoothly interpolates to the large regime where the model can be viewed as a zigzag SU() two-leg spin ladder. The phase exhibits both a -merized ground state and incommensurate spin-spin correlations. In stark contrast to the even case, we show that the -merized phase with odd only has a finite extent with no incommensuration. A gapless phase in the SU() universality class is stabilized for larger that stems from the existence of a massless renormalization group flow from SU() to SU() conformal field theories when is odd.
arXiv commentFinal version
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