Wilson-Polyakov Loop at Finite Temperature in Large N Gauge Theory and Anti-de Sitter Supergravity

Jung-Tay Yee; Soo-Jong Rey; Stefan Theisen

REVIEW

Wilson-Polyakov Loop at Finite Temperature in Large N Gauge Theory and Anti-de Sitter Supergravity

Soo-Jong Rey, Stefan Theisen, Jung-Tay Yee

High Energy Physics - Theory · Submitted 18 Mar 1998 · 23 references

Pith's verdict: The finite-temperature companion to Rey-Yee: a clean, first-principles Nambu-Goto computation whose only real soft spot is that the sharp screening cutoff at d* is a leading-order-in-N statement, which the paper never quite says out loud.

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arXiv IDhep-th/9803135 (version 2)

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CitationJung-Tay Yee, Soo-Jong Rey, Stefan Theisen. "Wilson-Polyakov Loop at Finite Temperature in Large N Gauge Theory and Anti-de Sitter Supergravity." arXiv:hep-th/9803135 (1998). https://pith.science/paper/57LTMBUI

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Editor's note

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This is the finite-temperature sequel to the authors' own zero-temperature Wilson loop paper, and it is the one that gave the field the screening length. The result is what you remember: a U-shaped string in Schwarzschild-AdS5, a maximum separation d_max, a crossover at d* below it, and a potential that is Coulomb-like at short distance and flat beyond d*. The elliptic-integral machinery in Eqs. (25)-(29) is dense but correct, and the asymptotic expansion Eq. (35) is the version everyone actually uses. The conformal scaling — V times d depends on T only through Td — is stated cleanly and is the part that made the paper useful to heavy-ion people. They also disclose the concurrent Witten and Brandhuber-Itzhaki-Sonnenschein-Yankielowicz papers and say plainly that Witten's no-phase-transition argument made them drop the deconfinement speculation from v1. That is the right way to handle a revision, and it should count in their favor. On the reader's main worry: I think it is misplaced. The claim that strings end at the horizon is not propped up only by the approximate probe-brane calculation in §3. In the static frame, H goes negative inside U0, so no static timelike worldsheet exists below the horizon; the endpoint is forced by the geometry. And §3's last paragraph upgrades the U = const solution of Eq. (40) to the exact condition U'^2 + H/G >= E^2, which the authors note is the same as the first integral Eq. (25). So §3 is a consistency check, not the load-bearing beam. The genuinely least-secure step is elsewhere: the sharp step at d* and the flat assertion on p. 4 that the straight-string pair carries no interaction energy. That is a leading-order statement in classical Nambu-Goto at large N; 1/N and string-loop corrections would smooth the step into a screening tail of the shape of Eq. (6). The paper is implicitly working at leading order, but it never says so, and a reader could mistake the step for an exact statement. That is a regime-of-validity caveat, not an error. The inside-horizon solution is presented without interpretation, which the authors admit; minor. Who should read it: anyone doing holographic QCD or finite-temperature AdS/CFT, and heavy-ion phenomenologists who want the origin of the screening length. It deserves a serious referee, and I would cite it.

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Major objections (3)

[§2, Eq. (35) and the following paragraph] The potential is quoted as exactly zero for d >= d*, and the text states that the straight-string pair 'has no interaction energy.' This is a leading-order statement in the classical Nambu-Goto/large-N expansion. The paper's own Eq. (6) predicts an exponentially screened tail from Debye-like screening, so the step at d* should be presented as the leading-order result, with the order in 1/N and 1/sqrt(g_eff) stated explicitly. As written, the abstract's claim of a 'finite range' (abstract:s2) reads as exact. Relatedly, Eq. (35) is derived from the large-a expansion of Eqs. (32)-(34) and is valid for d much less than d*, not for all d <= d* as the label suggests; the regime of validity should be corrected.
[§2, paragraph after Eq. (25) and Fig. 4; §3] Section 2 exhibits an explicit solution inside the horizon (the paragraph after Eq. (25) and Fig. 4), with real finite energy E(a,T) = 2U0 times the integral from 0 to 1 of sqrt((1-y^4)/(a^4-y^4)), while §3 concludes that configurations inside the horizon are unphysical because the electric field and energy become imaginary. The authors acknowledge that the interpretation of the inside-horizon solution is unclear and cite Minahan, but the two sections should be reconciled explicitly: either the inside-horizon solution should be labeled as a formal solution with no claimed physical interpretation, or the §3 conclusion should be qualified. As it stands, a reader can reasonably read the two sections as contradictory.
[§3 and §4] The probe-brane argument of §3 rests on the observation that H < 0 inside the horizon makes the electric field and energy imaginary. This is a statement about the static frame: below the horizon the Killing vector ∂_t is spacelike, so a static quark is not defined there in the first place. The conclusion that strings cannot penetrate the horizon is likely correct, but the clean argument is geometric — no static timelike worldsheet exists for U < U0 because h_00 = -α'U^2H/g_eff changes sign — and that argument should be stated directly in §2, where the horizon endpoint is actually used, rather than only in the approximate §3 analysis. In addition, the §4 statement that the horizon endpoint was 'crucial' overstates the dependence: the d-dependent terms of Eq. (35) come from the U-shape integral and are insensitive to the subtraction point; only the additive constant and the existence of the d > d* branch depend on where the straight string terminates.

Minor objections (7)

[Eq. (33)] The closed form sqrt(2)π^{3/2}/Γ(1/4)^2 evaluates to approximately 0.599, not 0.56 as quoted. Please check the decimal, since it propagates into the Coulomb coefficient 4c^2 in Eq. (35).
[Eq. (18) and the sentence following it] M^2 proportional to g_eff^2 would grow, not vanish, as g_eff goes to infinity, whereas the text states that M(r) vanishes in that limit. Please check the power of g_eff in Eq. (18).
[Abstract (abstract:s3) and §2] The conformal scaling is stated qualitatively. It would help to write the scaling law explicitly, for example V(d,T)d = f(Td), and to identify f from Eq. (35).
[Figures 2 and 3] The axes should state the units of d and V (presumably U0/g_eff and U0, respectively). The caption of Fig. 2 refers to (a^4-1)^{1/4} but the plotted horizontal variable is not identified.
[Reference list] Horowitz-Ooguri appears as both [7] and [21]; please merge or distinguish.
[Eqs. (20)-(21)] The physical interpretation of the thermal infrared divergence of the transverse fluctuations is not developed; is this a genuine instability of the straight-string configuration, or a gauge artifact? A sentence would help.
[Typographical] There are several typographical errors: 'gesults' (p.2), 'underyling' (p.2), 'obtaines' (p.6), 'ellictic' (p.9), and 'considerationa' (p.12).

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The paper

The paper claims

Using a string in a black-hole geometry, the authors argue that the force between a heavy quark and antiquark in a hot strongly coupled plasma is Coulomb-like at short range and then switches off entirely beyond a maximum separation.

The reading

The paper asks what becomes of the force between a heavy quark and its antiparticle once the surrounding gauge theory is heated past its deconfining transition. The authors work in the most tractable case available: maximally supersymmetric Yang–Mills theory with many colors at strong coupling, which is described by a string moving in five-dimensional anti-de Sitter space endowed with a black-hole horizon. The force is read off from the minimal surface swept by a string whose two ends sit on the boundary and are pulled apart, and the answer reported is a Coulomb-like attraction at short range that cuts off sharply beyond a maximum separation $d_*$. What makes this more than a curve fit is that the cutoff is not inserted by hand: it follows from the geometry, and the temperature dependence is fixed entirely by conformal invariance, so the result is a sharp statement about how a strongly coupled plasma screens color. The authors also use a probe brane carrying a single quark to argue that near-extremal branes and the strings ending on them sit at the horizon rather than falling through it.

What carries the argument

The load-bearing object is the U-shaped macroscopic string: a Nambu–Goto worldsheet whose two ends reach the anti-de Sitter boundary at separation $d$ and whose tip sits at $U_* = aU_0$, closest to the horizon. A first integral of the equations of motion, $(G/H)^2 U'^2 + GH = (g_{eff}^2/U_0^4)(1/a^4 - 1)$, reduces the problem to a one-dimensional mechanical analogue with conserved 'energy' set by $a$; the relation $d(a)$ and the regularized energy $E(d,T) - 2M_Q$ both come out as complete elliptic integrals of the first kind. The second ingredient is the competing configuration of two straight strings running from the boundary to the horizon at $U_0$, whose energy is exactly twice the quark mass and hence carries no interaction. Comparing the two energies produces the maximum distance $d_*$ and the sharp cutoff. A third ingredient, used only as supporting evidence, is the Born–Infeld Lagrangian of a probe D3-brane, where the metric function $H$ acts as a dielectric constant for an isolated quark's electric field and turns imaginary inside the horizon.

Extended reading notes

Core claim

The central claim is that the two-point correlator of Wilson–Polyakov loops at finite temperature, computed from the minimal Nambu–Goto action of a string in Schwarzschild–anti-de Sitter space, yields a heavy quark potential that is Coulomb-like at short distance and identically zero beyond a maximum separation. Concretely, for $d < d_*$ the potential is $V(d,T) = -4c^2 g_{eff}[1/d - U_0/(2c^2 g_{eff}) + (3/10)(U_0/(2c g_{eff}))^4 d^3 + ...]$ with $c = 0.56$ a ratio of complete elliptic integrals, and $V = 0$ for $d > d_*$; the transition happens because beyond $d_*$ a pair of straight, non-interacting strings has lower energy than the connected U-shaped string. The authors stress that the $1/d$ behavior has a different origin from the screened potential of ordinary QCD: here it comes from the underlying conformal invariance, which also forces $V$ times $d$ to depend on temperature only through the combination $Td$. They further report that the finite-temperature potential lies above the zero-temperature one at every distance, and that the temperature-dependent constant term in the bracket encodes the thermal correction.

Load-bearing premise

Everything hinges on the claim that the straight strings representing unpaired quarks terminate at the black-hole horizon rather than at the singularity, and the support for that is a probe-brane calculation the authors themselves describe as approximate, since an exact solution of the Born-Infeld equations was not found.

Editorial extensions

If this is right

For separations beyond $d_*$ the Polyakov loop correlator factorizes into a product of two independent loops, which is the geometric signature of the deconfined phase.
Because conformal invariance fixes the temperature dependence, the shape of the potential is universal up to rescaling by $T$, so the same curve should describe the theory at any temperature.
The finite-temperature potential sits above the zero-temperature Coulomb potential at every separation, so heating the theory always weakens the binding of the pair.
The straight-string configuration terminating at the horizon has zero interaction energy, giving a concrete geometric picture in which screening is a switch from a connected to a disconnected string rather than a Debye-style exponential.
The probe-brane argument, if accepted, implies that fundamental strings cannot penetrate the horizon, which constrains how black-hole interiors can be described by the dual gauge theory.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

If the horizon-termination picture holds, the same geometry should control screening of quarks in higher representations; hanging $k$ strings instead of one would give a $k$-dependent maximum separation, which is a check the paper does not perform.
The elliptic-integral structure that produces $d_{max}$ depends only on the existence of a horizon and a warp factor, so it should recur in any holographic background with a black brane, not just the conformal one studied here.
The paper's result is a strict strong-coupling statement; comparing its $1/d$ form with weak-coupling screened potentials would test whether any trace of the conformal behavior survives at intermediate coupling, though the two regimes are not continuously connected.
The authors note an additional solution branch inside the horizon whose interpretation they leave open; deciding whether it is a genuine saddle of the Euclidean action or a tunnelling configuration would clarify what, if anything, the gauge theory says about the region behind the horizon.

Original abstract

Aspects of d=4, N=4 superconformal U(N) gauge theory are studied at finite temperature. Utilizing dual description of large $N$ and strong coupling limit via Type IIB string theory compactification on Schwarzschild anti-de Sitter spacetime, we study correlations of Wilson-Polyakov loops and heavy quark potential thereof. We find that the heavy quark potential is Coulomb-like and has a finite range, as expected for gauge theory in high temperature, deconfinement phase. The potential exhibits finite temperature scaling consistent with underlying conformal invariance. We also study isolated heavy quark on probe D3-brane world-volume and find supporting evidence that near extremal D3-branes are located at Schwarzschild horizon.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,304 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.08 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.08 · compares with prior results 0.12 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; show every role.

Aspects of d=4, N=4 superconformal U(N) gauge theory are studied at finite temperature. Utilizing dual description of large $N$ and strong coupling limit via Type IIB string theory compactification on Schwarzschild anti-de Sitter spacetime, we study correlations of Wilson-Polyakov loops and heavy quark potential thereof. We find that the heavy quark potential is Coulomb-like and has a finite range, as expected for gauge theory in high temperature, deconfinement phase. The potential exhibits finite temperature scaling consistent with underlying conformal invariance. We also study isolated heavy quark on probe D3-brane world-volume and find supporting evidence that near extremal D3-branes are located at Schwarzschild horizon.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#	sentence	role	the authors' own work	states the main conclusion	strength
s0	Aspects of d=4, N=4 superconformal U(N) gauge theory are studied at finite temperature.	background 0.70	0.73	0.03	asserted 0.86
s1	Utilizing dual description of large $N$ and strong coupling limit via Type IIB string theory compactification on Schwarzschild anti-de Sitter spacetime, we study correlations of Wilson-Polyakov loops and heavy quark potential thereof.	method 0.75	0.84	0.07	asserted 0.92
s2	We find that the heavy quark potential is Coulomb-like and has a finite range, as expected for gauge theory in high temperature, deconfinement phase.	result 0.99	0.95	0.55	asserted 1.00
s3	The potential exhibits finite temperature scaling consistent with underlying conformal invariance.	result 0.79	0.83	0.13	asserted 0.82
s4	We also study isolated heavy quark on probe D3-brane world-volume and find supporting evidence that near extremal D3-branes are located at Schwarzschild horizon.	result 0.86	0.94	0.09	asserted 0.80

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.95.

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arXiv listing abstract v2

not examined

full text
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relations to other papers

levels run

P abstract

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S sections
T body sentences
C citations
R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures

**Figure 1.** Possible macroscopic string configurations representing various timelike PolyakovWilson loops at finite temperature. The Schwarzschild horizon is located at α ′U0. The first is a pair of straight, oppositely oriented strings stretched between the adS5 boundary and the Schwarzschild horizon. The second is a U-shaped string runnig between quark and anti-quark. The string tip is the closest point to the horizon and is located at aU0. For comparison, U-shape string at zero temperature is also shown. out of the adS5 boundary and acts as static color sources of the boundary…

**Figure 2.** Functional relation between the inter-quark distance d and (a 4 − 1)1/4 . For d ≤ dmax, the maximum inter-quark distance, there are two possible U-shape string configurations representing the Wilson-Polyakov loop correlator at two different values of a. Also illustrated for comparison is the same functional relation at zero temperature. Note that, at any d, the zero temperature configuration is always unique. where F(α, β) denotes an elliptic integral of the first kind. As in the zero temperature case, the parameter aU0 ≡ U∗ is the U-location for the tip of the U-shaped string.…

**Figure 3.** The heavy quark potential V(QQ)(d) defined in Eq. (31) as a function of interquark distance d. The upper dashed and the lower solid-dashed curves corresponds to two distinct string configurations for a given d ≤ dmax in

**Figure 4.** (a) string inside Schwarzschild horizon, (b) distance d versus first integral parameter a, (c) total energy as a function of d. Note the existence of a maximal distance dmax. = ± 1 4 √γ √ a 4 − 1 √ a 3 " F

Figures reproduced from arXiv:hep-th/9803135 by the authors.

References

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hep-th 2025-12 unverdicted novelty 5.0 of 10

Holographic minimal-surface calculation maps the Gross-Ooguri phase transition for circular Wilson loops on the Coulomb branch and indicates tree-level exactness for the straight line.
Quantum-Corrected Holographic Wilson Loop Expectation Values and Super-Yang-Mills Confinement
hep-th 2024-12 conditional novelty 5.0 of 10

Near-horizon quantum gravity fluctuations in an extremal AdS5-Reissner-Nordström black brane make the holographic Wilson loop obey an area law, producing a linear quark-antiquark potential at zero temperature.
Thermal entropy of a quark-antiquark pair above and below deconfinement from a dynamical holographic QCD model
hep-th 2017-08 conditional novelty 5.0 of 10

A holographic model with a temperature-carrying 'specious-confined' phase reproduces the lattice pattern of sharply rising quark-pair entropy near the deconfinement temperature, from both sides of the transition.
Energy loss, equilibration, and thermodynamics of a baryon rich strongly coupled quark-gluon plasma
hep-th 2015-07 conditional novelty 5.0 of 10

A holographic model fitted to zero-density lattice QCD predicts that heavy and light quark energy loss increases with baryon density and that equilibration is faster in a denser quark-gluon plasma.
Dynamical holographic QCD model for glueball and light meson spectra
hep-ph 2013-03 conditional novelty 5.0 of 10

A self-consistently deformed five-dimensional geometry, driven by a quadratic dilaton background, reproduces lattice glueball masses and light meson spectra within a single holographic model.
Strongly Coupled Gauge Theories: High and Low Temperature Behavior of Non-local Observables
hep-th 2012-12 conditional novelty 5.0 of 10

Using AdS/CFT, the authors derive analytic high- and low-temperature expansions for two-point functions, spatial Wilson loops, and entanglement entropy in strongly coupled gauge theories, showing exponential decay of ...
A hQCD model and its phase diagram in Einstein-Maxwell-Dilaton system
hep-th 2012-01 conditional novelty 5.0 of 10

A holographic QCD model with a quadratic warped factor and a U(1) charge yields a deconfinement phase diagram with a critical point at chemical potential about 0.34 GeV.
Thermodynamics of deformed AdS$_5$ model with a positive/negative quadratic correction in graviton-dilaton system
hep-th 2011-03 conditional novelty 5.0 of 10

A self-consistent black-hole solution for two deformed AdS5 models shows that bulk thermodynamics is insensitive to the sign of the quadratic correction, but the Polyakov loop and spatial string tension favor the posi...
Thermal Noise and Stochastic Strings in AdS/CFT
hep-th 2009-01 accept novelty 5.0 of 10

Integrating out string fluctuations behind a stretched horizon yields a stochastic boundary condition whose noise reproduces the boundary fluctuation-dissipation theorem and the bulk Kruskal two-point functions.
Universality of k-string Tensions from Holography and the Lattice
hep-th 2006-04 conditional novelty 5.0 of 10

Wilson loop expectation values in SU(N) gauge theory take the form dim R exp(-sigma_k A), with the string tension depending only on the N-ality k, not on the specific representation.
What RHIC Experiments and Theory tell us about Properties of Quark-Gluon Plasma ?
hep-ph 2004-05 conditional novelty 5.0 of 10

RHIC data show the quark-gluon plasma is a strongly coupled liquid with viscosity near the AdS/CFT bound, and the author argues it hosts hundreds of mostly colored bound states that shape its thermodynamics and jet quenching.
Thermodynamics of Heavy Quarkonium in a Bayesian Holographic QCD model
hep-ph 2025-08 conditional novelty 4.0 of 10

In a Bayesian holographic QCD model, rising temperature and baryon chemical potential lower the quarkonium dissociation distance and make binding energy vanish at smaller separation, promoting dissociation.
Why does the Quark-Gluon Plasma at RHIC behave as a nearly ideal fluid ?
hep-ph 2003-12 conditional novelty 4.0 of 10

The quark-gluon plasma made at RHIC is a strongly coupled liquid, not a weakly interacting gas, because near the critical temperature quasiparticles form loosely bound pairs that scatter strongly and drive viscosity d...
Dilatonic states, phase transitions, and criticality in holography
hep-th 2026-07 accept novelty 3.0 of 10

A review of holographic examples indicating that a light dilaton appears near critical endpoints of first-order zero-temperature phase transitions, with explicit but lower-dimensional demonstrations.
AdS/CFT Duality User Guide
hep-th 2014-09 accept novelty 3.0 of 10

A single-volume graduate textbook that teaches the AdS/CFT duality and its applications to quark-gluon plasma, hydrodynamics, and holographic superconductors, with worked computations and exercises.
Light-Front Holographic QCD and Emerging Confinement
hep-ph 2014-07 conditional novelty 3.0 of 10

A harmonic light-front confinement potential, fixed by a conformal-algebra construction and mapped to a soft-wall AdS dilaton, yields a massless pion and linear Regge trajectories with one fitted scale.
Heavy Quarkonium in Extreme Conditions
hep-ph 2019-12 accept novelty 2.0 of 10

The review consolidates a decade of theory showing that quarkonium in a hot QCD medium melts dynamically, through decoherence and medium-induced screening, rather than at sharp temperature thresholds.

How the literature uses it

86 arXiv papers cite this in 139 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 70 sentences without a confident label

Uses its method or tool 11 papers

If we in addition take the large $λ$ limit and use the AdS/CFT correspondence, the expectation value of the Wilson loop in the fundamental representation can be computed as [ref] W(C) = e^ i S_I, S_I = S(C) - 2 S_0 , where $S(C)$ is the Nambu-Goto action for the extremal worldsheet bounded at $z=0$ by the Wilson loop contour $C$ and $S_0$ is the Nambu-Goto action for an individual quark.

Robustness and Infrared Sensitivity of Various Observables in the Application of AdS/CFT to Heavy Ion Collisions · Calculation · 0.83
The second contribution on the r.h.s. of [ref] is the required counter-term which subtracts the very massive quark and antiquark contributions to the regularized potential and which takes in this case the following form ($ℓ=2r+2TT≫r≃2T$ and $M=U_max-U_T/2π$): [equation] Indeed, the "W-boson string" corresponds here to an open string stretched between the brane at $U_max$ and the Schwarzschild horizon $U=U_T$ [ref] .

Hadron potentials within the gauge/string correspondence · The conformal behaviour of the Wilson loop at finite temperature · 0.88
Standard techniques enable the computation of their separation distance and interaction potential [ref] .

Thermodynamics of Heavy Quarkonium in a Bayesian Holographic QCD model · The Setup · 0.88

Uses its data or values 2 papers

At $v=0$, $L_s^meson=0.28/T$ [ref] .

Velocity Dependence of Baryon Screening in a Hot Strongly Coupled Plasma · Introduction and Summary · 0.88
At $v=0$, $L_s=0.28/T$ [ref] .

Robustness and Infrared Sensitivity of Various Observables in the Application of AdS/CFT to Heavy Ion Collisions · Quark-Antiquark Potential and Screening Length · 0.81

Compares with it 10 papers

In the phase diagram of SYM theory, our new result can be interpreted as deforming the superconformal $𝒩=4$ SYM theory by finite chemical potential, in contrast to the finite-temperature deformation considered in [ref] .

Quantum-Corrected Holographic Wilson Loop Expectation Values and Super-Yang-Mills Confinement · Introduction · 0.89
One can see in figure 6 that there exists a maximal distance $l_max$ between the quark-anti-quark pair, a phenomenon already found in the study of the finite temperature Wilson line in the large $N$ limit of $U(N)$ $N = 4$ Super Yang-Mills theory in 4 dimensions [ref] - [ref] .

Holography and $AdS_4$ self-gravitating dyons · The Wilson loop · 0.98
This is a quite different behavior from the one which would be expected if there would be a classical AdS dual and $⟨W ⟩$ would be given in terms of a minimal surface in the AdS space [ref] [ref] [ref] .

A Systematic Study on Matrix Models for Chern-Simons-matter Theories · Introduction · 0.85

Cites it as support 1 paper

One concludes that only the lower part is physical [ref] .

Heavy quarks in the presence of higher derivative corrections from AdS/CFT · Numerical Solutions · 0.97

Cites it as background 40 papers

The potential for static heavy quarkonia at finite temperature in $𝒩=4$ super Yang-Mills theory was calculated via the methods of AdS/CFT by [ref] .

Bottomonia Suppression in Heavy Ion Collisions from AdS/CFT · Introduction · 0.95
The calculation of the free energy of a static pair in an $𝒩=4$ SYM plasma [ref] was among the first applications of the AdS/CFT correspondence.

Free Energy of a Heavy Quark-Antiquark Pair in a Thermal Medium from AdS/CFT · Introduction · 0.97
In the Maldacena limit of large-$N$ followed by $λ≫1$, the holographic dual of the fundamental representation Wilson line is a string anchored to the boundary of $AdS_5 ×S^5$ [ref] , which can be treated as a probe.

Holographic Entanglement Entropy of the Coulomb Branch · A simple example: the probe string · 0.89

Discussion

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