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Confinement on $\mathbb{R}^3 \times \mathbb{S}^1$ and Double-String Collapse
High Energy Physics - Theory · Submitted 9 Oct 2020
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We numerically study this mechanism and find that double-string confinement holds for strings of all $N$-alities, except for those between fundamental quarks.
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The abstract, sentence by sentence
We study confining strings in ${\cal{N}}=1$ supersymmetric $SU(N_c)$ Yang-Mills theory in the semiclassical regime on $\mathbb{R}^{1,2} \times \mathbb{S}^1$. Static quarks are expected to be confined by double strings composed of two domain walls - which are lines in $\mathbb{R}^2$ - rather than by a single flux tube. Each domain wall carries part of the quarks' chromoelectric flux. We numerically study this mechanism and find that double-string confinement holds for strings of all $N$-alities, except for those between fundamental quarks. We show that, for $N_c \ge 5$, the two domain walls confining unit $N$-ality quarks attract and form non-BPS bound states, collapsing to a single flux line. We determine the $N$-ality dependence of the string tensions for $2 \le N_c \le 10$. Compared to known scaling laws, we find a weaker, almost flat $N$-ality dependence, which is qualitatively explained by the properties of BPS domain walls. We also quantitatively study the behavior of confining strings upon increasing the $\mathbb{S}^1$ size by including the effect of virtual "$W$-bosons" and show that the qualitative features of double-string confinement persist.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study confining strings in ${\cal{N}}=1$ supersymmetric $SU(N_c)$ Yang-Mills theory in the semiclassical regime on $\mathbb{R}^{1,2} \times \mathbb{S}^1$. | contribution 0.81 | 0.88 | 0.04 | asserted 0.89 |
| s1 | Static quarks are expected to be confined by double strings composed of two domain walls - which are lines in $\mathbb{R}^2$ - rather than by a single flux tube. | background 0.90 | 0.09 | 0.19 | hedged possibility 0.97 |
| s2 | Each domain wall carries part of the quarks' chromoelectric flux. | background 0.95 | 0.12 | 0.04 | asserted 1.00 |
| s3 | We numerically study this mechanism and find that double-string confinement holds for strings of all $N$-alities, except for those between fundamental quarks. | result 0.99 | 0.97 | 0.35 | asserted 1.00 |
| s4 | We show that, for $N_c \ge 5$, the two domain walls confining unit $N$-ality quarks attract and form non-BPS bound states, collapsing to a single flux line. | result 1.00 | 0.94 | 0.34 | asserted 1.00 |
| s5 | We determine the $N$-ality dependence of the string tensions for $2 \le N_c \le 10$. | contribution 0.75 | 0.96 | 0.06 | asserted 0.99 |
| s6 | Compared to known scaling laws, we find a weaker, almost flat $N$-ality dependence, which is qualitatively explained by the properties of BPS domain walls. | result 0.85 | 0.97 | 0.14 | asserted 1.00 |
| s7 | We also quantitatively study the behavior of confining strings upon increasing the $\mathbb{S}^1$ size by including the effect of virtual "$W$-bosons" and show that the qualitative features of double-string confinement persist. | result 0.57 | 0.96 | 0.10 | asserted 1.00 |
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The paper
Original abstract
We study confining strings in ${\cal{N}}=1$ supersymmetric $SU(N_c)$ Yang-Mills theory in the semiclassical regime on $\mathbb{R}^{1,2} \times \mathbb{S}^1$. Static quarks are expected to be confined by double strings composed of two domain walls - which are lines in $\mathbb{R}^2$ - rather than by a single flux tube. Each domain wall carries part of the quarks' chromoelectric flux. We numerically study this mechanism and find that double-string confinement holds for strings of all $N$-alities, except for those between fundamental quarks. We show that, for $N_c \ge 5$, the two domain walls confining unit $N$-ality quarks attract and form non-BPS bound states, collapsing to a single flux line. We determine the $N$-ality dependence of the string tensions for $2 \le N_c \le 10$. Compared to known scaling laws, we find a weaker, almost flat $N$-ality dependence, which is qualitatively explained by the properties of BPS domain walls. We also quantitatively study the behavior of confining strings upon increasing the $\mathbb{S}^1$ size by including the effect of virtual "$W$-bosons" and show that the qualitative features of double-string confinement persist.
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References
How the literature uses it
4 arXiv papers cite this in 11 sentences
Papers citing it · 10 sentences without a confident label
Cites it as background 1 paper
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We can not discuss it any further and refer the reader to the literature (see [ref] , and, in a context related to our discussion, [ref] ; more references to the rather voluminous recent literature can be found there).[Let us mention also that there are phenomena related to the $θ=π$ domain walls and the deconfinement of probe quarks on their worldvolume whose unraveling demands going beyond the $μ≪1/L$ EFT, for example the braiding of fundamental Wilson loops on domain walls at $θ= π$ discussed in e.g. [ref] (this remark is also relevant for deconfinement on the QCD(adj) and SYM strings).
Notes on Confinement on $\mathbf{R^3 \times S^1}$: From Yang-Mills, super-Yang-Mills, and QCD(adj) to QCD(F) · $θ=π$: “double-string” confinement and deconfinement on domain walls. · 0.93
What it cites · 80 sentences without a confident label
Builds on 1 paper
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The novelty of this paper is to make use of the analytical results of [ref] classifying the BPS DW fluxes (and the further insight into their properties) in $SU(N>2)$ SYM to study the double-string confinement mechanism for $SU(N)$ SYM.
Domain walls and deconfinement: a semiclassical picture of discrete anomaly inflow · Relation To (and Differences From) Confinement in the $^3$ Polyakov Model · 0.98
Uses the method or tool of 3 papers
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The methods are mostly identical to those described in Sections 4 and 5 of [ref] , with some extensions and modifications.
Domain walls and deconfinement: a semiclassical picture of discrete anomaly inflow · Numerical Simulation of Double-String Configurations · 0.96
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We further investigated the attraction and repulsion of DWs by numerically relaxing configurations consisting of the sum of two DWs similar to those depicted in Figure [ref] (this way of studying DW interactions is motivated by the “streamline" or “valley" method of [ref] , see also [ref] ).
Instantons in QCD · Attraction and Repulsion of Domain Walls · 0.99
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Our computations for the confining string configurations were primarily performed on the Niagara cluster at the SciNet HPC Consortium [ref] .
Deploying a Top-100 Supercomputer for Large Parallel Workloads: the Niagara Supercomputer · Summary of Results and Outline · 0.95
Compares with 1 paper
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This qualitatively matches with a simple model of exponential DW repulsion proposed earlier for an $SU(2)$ theory [ref] .
Strings from domain walls in supersymmetric Yang-Mills theory and adjoint QCD · Summary of Results and Outline · 1.00
Cites as support 1 paper
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This is, in fact, necessitated by the new mixed discrete chiral/center symmetry anomaly, as discussed already in [ref] .
Domain walls and deconfinement: a semiclassical picture of discrete anomaly inflow · Relation To (and Differences From) Confinement in the $^3$ Polyakov Model · 0.98
Cites as background 20 papers
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But first, we remind the reader of the results of [ref] , which are essential for our arguments.
Domain walls and deconfinement: a semiclassical picture of discrete anomaly inflow · BPS DW Fluxes and Double-String Configurations · 0.81
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Of special interest to us in this paper is the theory formulated on $^3 ×^1$, with supersymmetric boundary conditions on $^1$ [ref] .
Aspects of N=2 Supersymmetric Gauge Theories in Three Dimensions · Introduction, Summary, and Outlook · 0.95
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Of special interest to us in this paper is the theory formulated on $^3 ×^1$, with supersymmetric boundary conditions on $^1$ [ref] .
Gauge Dynamics And Compactification To Three Dimensions · Introduction, Summary, and Outlook · 0.95
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