2018
DOI: 10.1103/physrevb.98.115163
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Deconfined criticality from the QED3 -Gross-Neveu model at three loops

Abstract: The QED3-Gross-Neveu model is a (2+1)-dimensional U(1) gauge theory involving Dirac fermions and a critical real scalar field. This theory has recently been argued to represent a dual description of the deconfined quantum critical point between Néel and valence bond solid orders in frustrated quantum magnets. We study the critical behavior of the QED3-Gross-Neveu model by means of an expansion around the upper critical space-time dimension of D + c = 4 up to the three-loop order. Estimates for critical exponen… Show more

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Cited by 33 publications
(34 citation statements)
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“…However, at smaller values of N f there is a discernible deviation amongst the various Padé approximants. A similar phenomenon was apparent for the chiral Ising QED-GNY theory [19,26] as well as for pure QED [17], whereas Padé approximants for pure GNY models are comparatively better behaved [46,57,72]. Physically this can be understood from the fact that the disordered phase of pure GNY models (a Dirac semimetal) is adiabatically connected to a system of noninteracting Dirac fermions regardless of the value of N f , whereas in QED-GNY models the disordered phase (the ASL) consists of a system of mutually interacting Dirac fermions and gauge fields which becomes increasingly strongly coupled in the infrared for small N f (at least in the sense of the 1/N f expansion).…”
Section: A Chiral Heisenberg Qed3-gny Modelsupporting
confidence: 67%
“…However, at smaller values of N f there is a discernible deviation amongst the various Padé approximants. A similar phenomenon was apparent for the chiral Ising QED-GNY theory [19,26] as well as for pure QED [17], whereas Padé approximants for pure GNY models are comparatively better behaved [46,57,72]. Physically this can be understood from the fact that the disordered phase of pure GNY models (a Dirac semimetal) is adiabatically connected to a system of noninteracting Dirac fermions regardless of the value of N f , whereas in QED-GNY models the disordered phase (the ASL) consists of a system of mutually interacting Dirac fermions and gauge fields which becomes increasingly strongly coupled in the infrared for small N f (at least in the sense of the 1/N f expansion).…”
Section: A Chiral Heisenberg Qed3-gny Modelsupporting
confidence: 67%
“…Looking forward, better algorithm in QMC simulations would certainly be desirable to access larger system sizes and lower temperatures. In particular, the critical properties of the U1D-VBS transition, that of the QED 3 -GN types, have already been discussed in the high-order perturbative RG calculations [42][43][44][45], but the system sizes in this work is too small to extract accurate values of the critical exponents. Further developments, in terms of algorithm improvement and more focus close to the QED 3 -GN critical points, are on-going.…”
Section: Conclusion and Discussionmentioning
confidence: 95%
“…The gapless excitation close to (π, 0) are the critical fluctuations associated with the QED 3 -GN transition. With larger system sizes and lower temperature in the future QMC studies, one will be able to measure the anomalous dimension exponent η from the momentum and frequency dependence of such critical fluctuation, and could compare with the predictions of QED 3 -GN transitions from the recent perturbative RG calculations [42][43][44][45].…”
Section: Dimer Spectra In Uid and Vbs Phasesmentioning
confidence: 99%
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“…The continuous confined transitions from U1D to AFM or VBS we found should be described by QED 3 -Gross-Neveu O (2) or O(3) universality, depending on the symmetry group that the fermion bilinears break in the confined phase, and further carefully study of the critical properties of these transitions via QMC simulations and analytical calculations is certainly worthwhile [93]. Recently perturbative renormalization group calculations to higher orders have been carried out in attempt to accquire the critical properties of the deconfinement to confinement transition in form of QED 3 -Gross-Neveu universality classes [120][121][122][123][124][125] and to address the relevance or irrelevance of the monopole operators to the stability of the U1D phase [126][127][128], show substantial interests and great ongoing efforts along this direction.…”
Section: A Dirac Fermions Coupled With Phononsmentioning
confidence: 99%