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Topological susceptibility from the twisted mass Dirac operator spectrum
High Energy Physics - Lattice · Submitted 18 Dec 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We present results of our computation of the topological susceptibility with $N_f=2$ and $N_f=2+1+1$ flavours of maximally twisted mass fermions, using the method of spectral projectors.
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The abstract, sentence by sentence
We present results of our computation of the topological susceptibility with $N_f=2$ and $N_f=2+1+1$ flavours of maximally twisted mass fermions, using the method of spectral projectors. We perform a detailed study of the quark mass dependence and discretization effects. We make an attempt to confront our data with chiral perturbation theory and extract the chiral condensate from the quark mass dependence of the topological susceptibility. We compare the value with the results of our direct computation from the slope of the mode number. We emphasize the role of autocorrelations and the necessity of long Monte Carlo runs to obtain results with good precision. We also show our results for the spectral projector computation of the ratio of renormalization constants $Z_P/Z_S$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present results of our computation of the topological susceptibility with $N_f=2$ and $N_f=2+1+1$ flavours of maximally twisted mass fermions, using the method of spectral projectors. | contribution 0.96 | 0.97 | 0.13 | asserted 1.00 |
| s1 | We perform a detailed study of the quark mass dependence and discretization effects. | contribution 0.89 | 0.96 | 0.04 | asserted 0.94 |
| s2 | We make an attempt to confront our data with chiral perturbation theory and extract the chiral condensate from the quark mass dependence of the topological susceptibility. | contribution 0.78 | 0.94 | 0.11 | hedged possibility 0.67 |
| s3 | We compare the value with the results of our direct computation from the slope of the mode number. | contribution 0.41 | 0.93 | 0.10 | asserted 0.98 |
| s4 | We emphasize the role of autocorrelations and the necessity of long Monte Carlo runs to obtain results with good precision. | limitation 0.60 | 0.66 | 0.07 | asserted 1.00 |
| s5 | We also show our results for the spectral projector computation of the ratio of renormalization constants $Z_P/Z_S$. | result 0.76 | 0.97 | 0.05 | asserted 1.00 |
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The paper
Original abstract
We present results of our computation of the topological susceptibility with $N_f=2$ and $N_f=2+1+1$ flavours of maximally twisted mass fermions, using the method of spectral projectors. We perform a detailed study of the quark mass dependence and discretization effects. We make an attempt to confront our data with chiral perturbation theory and extract the chiral condensate from the quark mass dependence of the topological susceptibility. We compare the value with the results of our direct computation from the slope of the mode number. We emphasize the role of autocorrelations and the necessity of long Monte Carlo runs to obtain results with good precision. We also show our results for the spectral projector computation of the ratio of renormalization constants $Z_P/Z_S$.
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References
How the literature uses it
16 arXiv papers cite this in 23 sentences
Papers citing it · 13 sentences without a confident label
Uses its method or tool 3 papers
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This quantity can be computed from spectral methods using the eigenvectors obtained from the same eigenvalue problem in Eq. [ref] [ref] as follows:
Nonperturbative determination of the ${\cal N} = 1$ supersymmetric Yang-Mills gluino condensate at large $N$ · Spectral method (Banks–Casher) · 1.00
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In order to compute $χ_∞$, we use the method of spectral projectors [ref] .
Testing the Witten-Veneziano Formula on the Lattice · Quenched $χ_∞$ · 1.00
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We follow the strategy presented in Ref. [ref] to extract the value of $Z_P/Z_S$ for each ensemble, i.e. we take the central value to be the one corresponding to some large value of $r_0 M$, chosen as 1.5, in order to avoid contamination by non-perturbative effects appearing for small $r_0 M$.
Non-perturbative Test of the Witten-Veneziano Formula from Lattice QCD · Computation of ZP over ZS · 1.00
Uses its data or values 1 paper
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The results that they have obtained in the $N_f=2+1+1$ theory is shown in the right plot of Figure [ref] as a function of the renormalized quark mass [ref] .
Recent progress on chiral symmetry breaking in QCD · Topological susceptibility in QCD · 0.92
Compares with it 2 papers
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We also note that the scaling pattern we observe is quite comparable with those reported by the ETMC at zero temperature in their study of the topological susceptibility from the twisted mass Dirac operator spectrum [ref] .
Chiral observables and topology in hot QCD with two families of quarks · Details on lattice artifacts · 1.00
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Our results are summarized in Fig. [ref] (see also Fig. [ref] for a comparison with Ref. [ref] and Ref. [ref] ).
Topological susceptibility of QCD with dynamical M\"obius domain wall fermions · Results at high beta · 1.00
Cites it as background 4 papers
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Apart from the link to the chiral condensate, the Dirac spectrum is also related to the topological susceptibility [ref] and the quark mass anomalous dimension.
Quark mass anomalous dimension and $\Lambda_{\overline{\textrm{MS}}}$ from the twisted mass Dirac operator spectrum · Introduction · 0.89
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Lattice QCD simulations have provided information on $θ$-dependence below [ref] and across the deconfinement temperature $T_c$ [ref] since long, and the interest related to axion physics has fostered renewed efforts from the lattice community in the recent past [ref] .
Topology in full QCD at high temperature: a multicanonical approach · Introduction · 0.96
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It should be also noted that the spectral method has been extensively used in the QCD literature [ref] .
Nonperturbative determination of the ${\cal N} = 1$ supersymmetric Yang-Mills gluino condensate at large $N$ · Methods · 0.90
What it cites · 24 sentences without a confident label
Builds on 1 paper
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This definition of the topological susceptibility was subject to numerical analysis in the quenched case [ref] and it is the aim of the present paper to analyze the results of its usage in the case with $N_f=2$ and $N_f=2+1+1$ active flavours of twisted mass fermions.
Universality of the topological susceptibility in the SU(3) gauge theory · Introduction · 0.96
Uses the method or tool of 2 papers
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The method that we follow in this paper was introduced in Refs. [ref] and we refer to these papers for a comprehensive description.
Chiral symmetry breaking and the Banks--Casher relation in lattice QCD with Wilson quarks · Theoretical principles · 0.99
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The method that we follow in this paper was introduced in Refs. [ref] and we refer to these papers for a comprehensive description.
Universality of the topological susceptibility in the SU(3) gauge theory · Theoretical principles · 0.99
Compares with 3 papers
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Still, our result is in agreement with the direct determination from the mode number on the same set of gauge field ensembles – $r_0 Σ^1/3 = 0.680(20)(21)$ [ref] , indicating that LO$χ$PT describes the quark mass dependence of the topological susceptibility at least within the rather large errors of our results.
Chiral condensate from the twisted mass Dirac operator spectrum · $N_f=2+1+1$ results · 0.93
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For all these ensembles, we can compare the values of $Z_P/Z_S$ with an alternative computation – in the framework of the RI-MOM renormalization scheme ($β=3.9, 4.05, 4.2$ [ref] ) or the X-space renormalization scheme ($β=4.35$ [ref] ).
Non-perturbative renormalization in coordinate space for $N_f=2$ maximally twisted mass fermions with tree-level Symanzik improved gauge action · $N_f=2$ · 0.97
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For all these ensembles, we can compare the values of $Z_P/Z_S$ with an alternative computation – in the framework of the RI-MOM renormalization scheme ($β=3.9, 4.05, 4.2$ [ref] ) or the X-space renormalization scheme ($β=4.35$ [ref] ).
Renormalization constants of local operators for Wilson type improved fermions · $N_f=2$ · 0.97
Cites as background 1 paper
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There exist many definitions of the topological charge on the lattice[For a short review and discussion of different definitions and for further references, we refer to Ref. [ref] .] and there has been a debate in the literature about the validity of different approaches.
Anomalies, gauge field topology, and the lattice · Introduction · 1.00
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