2021
DOI: 10.1016/j.nuclphysb.2020.115241
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Random-mass disorder in the critical Gross-Neveu-Yukawa models

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Cited by 13 publications
(11 citation statements)
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“…However, if degeneracies such as spin or valley pseudo-spin are included, the clean fixed point becomes stable against weak bosonic mass disorder and a finite-disorder multicritical point with noninteger dynamical exponent (z > 1) can be identified within the double expansion [40]. Similar finite disorder fixed points were established in the chiral Ising and Heisenberg GNY models with bosonic random-mass disorder, using triple expansion [41].…”
Section: Introductionmentioning
confidence: 56%
“…However, if degeneracies such as spin or valley pseudo-spin are included, the clean fixed point becomes stable against weak bosonic mass disorder and a finite-disorder multicritical point with noninteger dynamical exponent (z > 1) can be identified within the double expansion [40]. Similar finite disorder fixed points were established in the chiral Ising and Heisenberg GNY models with bosonic random-mass disorder, using triple expansion [41].…”
Section: Introductionmentioning
confidence: 56%
“…However, if degeneracies such as spin or valley pseudo-spin are included, the clean fixed point becomes stable against weak bosonic mass disorder and a finite-disorder multi-critical point with non-integer dynamical exponent (z > 1) can be identified within the double expansion [39]. Similar finite disorder fixed points were established in the chiral Ising and Heisenberg GNY models with bosonic random-mass disorder, using triple expansion [40].…”
Section: Introductionmentioning
confidence: 58%
“…The interplay between symmetry breaking and disorder was previously studied for the XY GNY [38,39] and the chiral Ising and Heisenberg GNY models [40], using the replica formalism combined with expansions. Near the upper critical dimension fermionic disorder is strongly irrelevant at the clean system quantum critical points.…”
Section: Discussionmentioning
confidence: 99%
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