2018
DOI: 10.1103/physrevd.98.096005
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Critical Wess-Zumino models with four supercharges in the functional renormalization group approach

Abstract: We analyze the N = 1 supersymmetric Wess-Zumino model dimensionally reduced to the N = 2 supersymmetric model in three Euclidean dimensions. As in the original model in four dimensions and the N = (2, 2) model in two dimensions the superpotential is not renormalized. This property puts severe constraints on the non-trivial fixed-point solutions, which are studied in detail. We admit a field-dependent wave function renormalization that in a geometric language relates to a Kähler metric. The Kähler metric is not… Show more

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Cited by 13 publications
(15 citation statements)
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References 132 publications
(181 reference statements)
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“…Concomitant with the topological phase transition from second-order to topological insulator, time-reversal symmetry and inversion symmetry emerge. The previous works has shown the possibility of emergent Lorentz symmetry [63][64][65][66][67][68][69][70], emergent chiral symmetry [71][72][73], and even emergent supersymmetry [74][75][76][77][78][79][80][81][82][83][84][85]. Here, by providing the concrete example, we show that emergent symmetries could happen for the discrete time-reversal and inversion symmetries, which enrich the family of emergent symmetries [86].…”
supporting
confidence: 50%
“…Concomitant with the topological phase transition from second-order to topological insulator, time-reversal symmetry and inversion symmetry emerge. The previous works has shown the possibility of emergent Lorentz symmetry [63][64][65][66][67][68][69][70], emergent chiral symmetry [71][72][73], and even emergent supersymmetry [74][75][76][77][78][79][80][81][82][83][84][85]. Here, by providing the concrete example, we show that emergent symmetries could happen for the discrete time-reversal and inversion symmetries, which enrich the family of emergent symmetries [86].…”
supporting
confidence: 50%
“…The key features of the FRG approach in the present context are the following: The FRG is well-suited for calculations directly in 2+1 dimensions. It has been tested against other methods which has shown that it provides very good results in the context of Gross-NeveuYukawa models [46][47][48][49][50][51][52][53][54][55][56][57][58][59][60] . Importantly, the FRG approach already includes resummation effects through the non-perturbative threshold functions 61,62 , which is in contrast to perturbative approaches.…”
Section: A Methodsmentioning
confidence: 99%
“…(2) The conformal bootstrap has emerged as a numerical tool to determine critical exponents for fermionic models [43][44][45][46]. (3) Nonperturbative field-theoretical methods like the functional renormalization group (FRG) have managed to explore sophisticated truncation schemes [47][48][49][50][51][52]. (4) The perturbative renormalization group (pRG) has seen substantial advances in computational technology and the development of suitable algorithms which facilitate the calculation of higherloop orders.…”
Section: Introductionmentioning
confidence: 99%