2021
DOI: 10.1103/physrevb.104.205142
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Self-duality protected multicriticality in deconfined quantum phase transitions

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Cited by 18 publications
(19 citation statements)
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“…The DQCP has long been associated with unconventional phenomena including fractional spinon excitations and deconfined gauge fluctuations [3][4][5], and further intensive investigation of the DQCP scenario has introduced emergent symmetries [6][7][8][9][10] and exotic firstorder transitions [11,12]. In a very recent scenario, the DQCP is multi-critical [13,14] and generically connected to a gapless quantum spin liquid (QSL) [15][16][17][18][19].…”
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confidence: 99%
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“…The DQCP has long been associated with unconventional phenomena including fractional spinon excitations and deconfined gauge fluctuations [3][4][5], and further intensive investigation of the DQCP scenario has introduced emergent symmetries [6][7][8][9][10] and exotic firstorder transitions [11,12]. In a very recent scenario, the DQCP is multi-critical [13,14] and generically connected to a gapless quantum spin liquid (QSL) [15][16][17][18][19].…”
mentioning
confidence: 99%
“…The 2D S = 1/2 Heisenberg model with uniform frustrated interactions on square-lattice offers a more frequently studied close analogy to the SSM, though hosting a four-fold degenerate dimerized phase in place of the two-fold degenerate PS phase of the SSM. A QSL phase exists in an extended parameter space between the dimerized and AFM phases [15,19,[38][39][40] and terminates at a DQCP with emergent SO(5) symmetry [14,16,17]. Beyond the DQCP, the direct PS-AFM transition is expected to be first-order, with the coexistence state inheriting (and breaking) the emergent symmetry of the DQCP [7][8][9]14].…”
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confidence: 99%
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“…When a duality becomes a symmetry (i.e., the system is self-dual ), the self-duality must force the system to stay on the phase boundary between the two duality-related phases, often leading to criticality or multicriticality [18][19][20][21]. A prominent example is the quantum transverse field Ising chain H Ising = − j (σ z j σ z j+1 + hσ x j ), in which the Kramers-Wannier duality [22,23] exchanges the symmetric phase and the Z 2 SSB phase.…”
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confidence: 99%