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S. Benvenuti and H. Khachatryan, “Easy-plane QED 3 ’s in the large N f N_{f} limit,” arXiv:1902.05767 [hep-th]
Original
1902
Earlier work this paper cites.
A. V. Kotikov and S. Teber, “Addendum to ”Critical behaviour of ( 2 + 1 2+1 )-dimensional QED: 1 / N f 1/N_{f} -corrections in an arbitrary non-local gauge”,” arXiv:1902.03790 [hep-th]
Original
1902
Earlier work this paper cites.
A.N. Vasil’ev, M.Yu. Nalimov, “The C P N − 1 CP^{N-1} model: Calculation of anomalous dimensions and the mixing matrices in the order 1/N,” Theor. Math. Phys. (1983) 56: 643. https://doi.org/10.1007/BF01027537
1983
Earlier work this paper cites.
R. D. Pisarski, “Chiral Symmetry Breaking in Three-Dimensional Electrodynamics,” Phys. Rev. D 29
1984
Earlier work this paper cites.
G. Murthy and S. Sachdev, “Action of Hedgehog Instantons in the Disordered Phase of the (2+1)-dimensional CP**( 1
1990
Earlier work this paper cites.
J. March-Russell, “On the possibility of second order phase transitions in spontaneously broken gauge theories,” Phys. Lett. B 296
1992
Earlier work this paper cites.
J. A. Gracey, “Electron mass anomalous dimension at O(1/(Nf(2)) in quantum electrodynamics,” Phys. Lett. B 317
1993
Earlier work this paper cites.
J. A. Gracey, “Gauged Nambu-Jona-Lasinio model at O(1/N) with and without a Chern-Simons term,” Mod. Phys. Lett. A 8
1993
Earlier work this paper cites.
V. Borokhov, A. Kapustin and X. k. Wu, “Topological disorder operators in three-dimensional conformal field theory,” JHEP 0211
2002
Earlier work this paper cites.
P. Calabrese, A. Pelissetto and E. Vicari, “Multicritical phenomena in O(n(1)) + O(n(2)) symmetric theories,” Phys. Rev. B 67
2003
Earlier work this paper cites.
T. Senthil, A. Vishwanath, L. Balents, S. Sachdev, M.P.A. Fisher, “”Deconfined” quantum critical points,” Science 303, 1490 (2004) doi:10.1126/science.1091806 [arXiv:cond-mat/0311326 [cond-mat.str-el]]
2004
Earlier work this paper cites.
K. Kaveh and I. F. Herbut, “Chiral symmetry breaking in QED(3) in presence of irrelevant interactions: A Renormalization group study,” Phys. Rev. B 71
2005
Earlier work this paper cites.
R. K. Kaul and S. Sachdev, “Quantum criticality of U(1) gauge theories with fermionic and bosonic matter in two spatial dimensions,” Phys. Rev. B 77
Original
2008
Earlier work this paper cites.
O. Aharony, G. Gur-Ari and R. Yacoby, “d=3 Bosonic Vector Models Coupled to Chern-Simons Gauge Theories,” JHEP 1203
Original
2012
Earlier work this paper cites.
S. Giombi, S. Minwalla, S. Prakash, S. P. Trivedi, S. R. Wadia and X. Yin, “Chern-Simons Theory with Vector Fermion Matter,” Eur. Phys. J. C 72
Original
2012
Earlier work this paper cites.
O. Aharony, G. Gur-Ari and R. Yacoby, “Correlation Functions of Large N Chern-Simons-Matter Theories and Bosonization in Three Dimensions,” JHEP 1212
Original
2012
Earlier work this paper cites.
R. K. Kaul and A. W. Sandvik, “Lattice Model for the SU ( N ) (N) Nèel to Valence-Bond Solid Quantum Phase Transition at Large N N ,” Phys. Rev. Lett. 108
Original
2012
Earlier work this paper cites.
I. R. Klebanov, S. S. Pufu, S. Sachdev and B. R. Safdi, “Entanglement Entropy of 3-d Conformal Gauge Theories with Many Flavors,” JHEP 1205
Original
2012
Earlier work this paper cites.
F. S. Nogueira and A. Sudbo, “Deconfined Quantum Criticality and Conformal Phase Transition in Two-Dimensional Antiferromagnets,” EPL 104
Original
2013
Earlier work this paper cites.
S. S. Pufu, “Anomalous dimensions of monopole operators in three-dimensional quantum electrodynamics,” Phys. Rev. D 89
Original
2014
Earlier work this paper cites.
J. Braun, H. Gies, L. Janssen and D. Roscher, “Phase structure of many-flavor QED 3 ,” Phys. Rev. D 90
Original
2014
Earlier work this paper cites.
D. T. Son, “Is the Composite Fermion a Dirac Particle?,” Phys. Rev. X 5
Original
2015
Earlier work this paper cites.

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Original
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Later among the works it cites.
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Original
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Later among the works it cites.
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Later among the works it cites.
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2018

QED's in $2{+}1$ dimensions: complex fixed points and dualities

Benvenuti, Sergio, Khachatryan, Hrachya

Understand

We consider Quantum Electrodynamics with an even number $N_f$ of bosonic or fermionic flavors, allowing for interactions respecting at least $U(N_f/2)^2$ global symmetry.

Both in the bosonic and in the fermionic case, we find four interacting fixed points: two with $U(N_f/2)^2$ symmetry, two with $U(N_f)$ symmetry.
Large $N_f$ arguments suggest that, lowering $N_f$, all these fixed points merge pairwise and become complex CFT's.
In the bosonic QED's the merging happens around $N_f\sim 9{-}11$ and does not break the global symmetry.