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Fermion-induced quantum critical points in two-dimensional Dirac semimetals
Strongly Correlated Electrons · Submitted 24 Oct 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim From large-$N$ renormalization group (RG) analysis, we find that fermion-induced quantum critical points (FIQCPs) [Z.-X.
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In this paper we investigate the nature of quantum phase transitions between two-dimensional Dirac semimetals and $Z_3$-ordered phases (e.g. Kekule valence-bond solid), where cubic terms of the order parameter are allowed in the quantum Landau-Ginzberg theory and the transitions are putatively first-order. From large-$N$ renormalization group (RG) analysis, we find that fermion-induced quantum critical points (FIQCPs) [Z.-X. Li et al., Nature Communications 8, 314 (2017)] occur when $N$ (the number of flavors of four-component Dirac fermions) is larger than a critical value $N_c$. Remarkably, from the knowledge of spacetime supersymmetry, we obtain an exact lower bound for $N_c$, i.e., $N_c>1/2$. (Here the "1/2" flavor of four-component Dirac fermions is equivalent to one flavor of four-component Majorana fermions). Moreover, we show that the emergence of two length scales is a typical phenomenon of FIQCPs and obtain two different critical exponents, i.e., $\nu$$\neq$$\nu'$, by large-$N$ RG calculations. We further give a brief discussion on possible experimental realizations of FIQCPs.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper we investigate the nature of quantum phase transitions between two-dimensional Dirac semimetals and $Z_3$-ordered phases (e.g. Kekule valence-bond solid), where cubic terms of the order parameter are allowed in the quantum Landau-Ginzberg theory and the transitions are putatively first-order. | contribution 0.69 | 0.52 | 0.08 | hedged possibility 0.77 |
| s1 | From large-$N$ renormalization group (RG) analysis, we find that fermion-induced quantum critical points (FIQCPs) [Z.-X. | result 0.73 | 0.91 | 0.31 | asserted 0.97 |
| s2 | Li et al., Nature Communications 8, 314 (2017)] occur when $N$ (the number of flavors of four-component Dirac fermions) is larger than a critical value $N_c$. | result 0.96 | 0.73 | 0.29 | asserted 1.00 |
| s3 | Remarkably, from the knowledge of spacetime supersymmetry, we obtain an exact lower bound for $N_c$, i.e., $N_c>1/2$. | result 0.99 | 0.90 | 0.24 | asserted 1.00 |
| s4 | (Here the "1/2" flavor of four-component Dirac fermions is equivalent to one flavor of four-component Majorana fermions). | interpretation 0.91 | 0.38 | 0.06 | asserted 0.98 |
| s5 | Moreover, we show that the emergence of two length scales is a typical phenomenon of FIQCPs and obtain two different critical exponents, i.e., $\nu$$\neq$$\nu'$, by large-$N$ RG calculations. | result 1.00 | 0.96 | 0.22 | asserted 1.00 |
| s6 | We further give a brief discussion on possible experimental realizations of FIQCPs. | future work 0.62 | 0.75 | 0.04 | hedged possibility 0.80 |
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Original abstract
In this paper we investigate the nature of quantum phase transitions between two-dimensional Dirac semimetals and $Z_3$-ordered phases (e.g. Kekule valence-bond solid), where cubic terms of the order parameter are allowed in the quantum Landau-Ginzberg theory and the transitions are putatively first-order. From large-$N$ renormalization group (RG) analysis, we find that fermion-induced quantum critical points (FIQCPs) [Z.-X. Li et al., Nature Communications 8, 314 (2017)] occur when $N$ (the number of flavors of four-component Dirac fermions) is larger than a critical value $N_c$. Remarkably, from the knowledge of spacetime supersymmetry, we obtain an exact lower bound for $N_c$, i.e., $N_c>1/2$. (Here the "1/2" flavor of four-component Dirac fermions is equivalent to one flavor of four-component Majorana fermions). Moreover, we show that the emergence of two length scales is a typical phenomenon of FIQCPs and obtain two different critical exponents, i.e., $\nu$$\neq$$\nu'$, by large-$N$ RG calculations. We further give a brief discussion on possible experimental realizations of FIQCPs.
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How the literature uses it
5 arXiv papers cite this in 9 sentences
Papers citing it · 6 sentences without a confident label
Compares with it 1 paper
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This lies in the range of upper and lower bounds obtained by QMC calculations [ref] , $N_f,c<2$, and an emergent SUSY theory [ref] , $N_f,c>1/2$.
Fermion-induced quantum criticality in two-dimensional Dirac semimetals: Non-perturbative flow equations, fixed points and critical exponents · Fixed point stability for varying numbers of fermions · 0.95
Cites it as background 2 papers
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Recently, based on the 2D and 3D semimetal, the fermion-boson mixed system was proposed to describe the Landau-forbidden quantum phase transition, which gives rise to Fermion-induced quantum critical points(FIQCP) [ref] and fluctuation-induced continuous phase transition with hidden degrees of freedom [ref] .
Duality of deconfined quantum critical point in two dimensional Dirac semimetals · Introduction · 0.81
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This category of QCP always occurs in the interacting systems with Dirac and Weyl excitations [ref] , such as graphene superconducting criticality [ref] , emergent supersymmetric criticality on the surface of three-dimensional (3D) topological insulators [ref] , fermion-induced quantum criticality in Weyl or Dirac semimetals [ref] .
Critical behavior of QED$_3$--Gross-Neveu-Yukawa Theory in an Arbitrary Gauge · Introduction · 0.90
What it cites · 2 sentences without a confident label
Uses the method or tool of 2 papers
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In this paper, with the help of spacetime supersymmetry (SUSY) [ref] , we can show exactly that for $N=1/2$ such a $Z_3$ Gross-Neveu-Yukawa transition must be first-order.
An Unorthodox Introduction to Supersymmetric Gauge Theory · Introduction · 0.84
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In this paper, with the help of spacetime supersymmetry (SUSY) [ref] , we can show exactly that for $N=1/2$ such a $Z_3$ Gross-Neveu-Yukawa transition must be first-order.
The Power of Holomorphy -- Exact Results in 4D SUSY Field Theories · Introduction · 0.84
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