REVIEW
Novel Local CFT and Exact Results on Perturbations of N=4 Super Yang Mills from AdS Dynamics
High Energy Physics - Theory · Submitted 16 Oct 1998 · 29 references
Pith's verdict: The interpolating-flow construction and the monotonic c(x) are the durable contributions; the 'new CFTs' claim leans on a 10d lift the paper only calls 'most probably' true, and the Addendum quietly halves it.
T0 · AI review
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Referee report
The paper
The paper claims
Two non-supersymmetric AdS5 stationary points of five-dimensional gauged supergravity are argued to be new local conformal field theories, connected to N=4 super Yang-Mills by interpolating holographic renormalization-group flows.
The reading
Extended reading notes
Core claim
The abstract states: 'We find new, local, non-supersymmetric conformal field theories obtained by relevant deformations of the N=4 super Yang Mills theory in the large N limit,' backed by 'interpolating supergravity solutions that naturally represent the flow from the N=4 super Yang Mills UV theory to these non-supersymmetric IR fixed points.' If correct, two new conformal fixed points exist and are connected to N=4 by genuine renormalization-group trajectories realized as classical supergravity solutions.
Load-bearing premise
The interpretation of the five-dimensional stationary points as four-dimensional conformal field theories rests on the claim that they lift to full ten-dimensional Type IIB compactifications. Section 4 says of the stationary points that 'they are most probably true compactifications of Type IIB supergravity [16, 17].' The word 'probably' is doing load-bearing work: locality and the CFT interpretation are argued from these lifts, and the paper does not construct the ten-dimensional solution itself.
Original abstract
We find new, local, non-supersymmetric conformal field theories obtained by relevant deformations of the N=4 super Yang Mills theory in the large $N$ limit. We contruct interpolating supergravity solutions that naturally represent the flow from the N=4 super Yang Mills UV theory to these non-supersymmetric IR fixed points. We also study the linearization around the N=4 superconformal point of N=1 supersymmetric, marginal deformations. We show that they give rise to N=1 superconformal fixed points, as expected from field-theoretical arguments.
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.
The abstract, sentence by sentence
We find new, local, non-supersymmetric conformal field theories obtained by relevant deformations of the N=4 super Yang Mills theory in the large $N$ limit. We contruct interpolating supergravity solutions that naturally represent the flow from the N=4 super Yang Mills UV theory to these non-supersymmetric IR fixed points. We also study the linearization around the N=4 superconformal point of N=1 supersymmetric, marginal deformations. We show that they give rise to N=1 superconformal fixed points, as expected from field-theoretical arguments.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We find new, local, non-supersymmetric conformal field theories obtained by relevant deformations of the N=4 super Yang Mills theory in the large $N$ limit. | result 0.93 | 0.96 | 0.72 | asserted 1.00 |
| s1 | We contruct interpolating supergravity solutions that naturally represent the flow from the N=4 super Yang Mills UV theory to these non-supersymmetric IR fixed points. | contribution 0.73 | 0.95 | 0.18 | asserted 1.00 |
| s2 | We also study the linearization around the N=4 superconformal point of N=1 supersymmetric, marginal deformations. | contribution 0.96 | 0.92 | 0.07 | asserted 0.84 |
| s3 | We show that they give rise to N=1 superconformal fixed points, as expected from field-theoretical arguments. | result 0.87 | 0.89 | 0.19 | asserted 1.00 |
What was examined, and what was not
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Figures
Figures reproduced from arXiv:hep-th/9810126 by the authors.
References
How later papers used it
129 later papers cite it
2 later papers by other authors are listed below: 1 used its method or tool and 1 compared its own results with it.
Uses its method or tool 1 of 4 papers with this label
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Calculated the central charge c following the prescription developed in this paper.
A tale of two cascades: Higgsing and Seiberg-duality cascades from type IIB string theory (2011) · 1.00 · paraphrased: the licence does not allow quoting
Compares with it 1 of 3 papers with this label
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Said that its analysis is equivalent to this paper's, provided the central charge function is identified as c(z) ∼ (T_zz)^-5/2.
A new 6d fixed point from holography (2016) · 0.85 · paraphrased: the licence does not allow quoting
How the literature uses it
124 arXiv papers cite this in 164 sentences
Papers citing it · 103 sentences without a confident label
Uses its method or tool 4 papers
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We calculate the central charge $c$, following the prescription developed in [ref] , [ref] .
A tale of two cascades: Higgsing and Seiberg-duality cascades from type IIB string theory · Central Charge · 1.00
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We should follow the usual procedure of [ref] , that requires a reduction to five dimensions.
The Non-SUSY Baryonic Branch: Soft Supersymmetry Breaking of N=1 Gauge Theories · Central charge · 0.99
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When looking for holographic $c$-functions, another option is applying the standard prescription [ref] in global coordinates.
AdS Vacuum Bubbles, Holography and Dual RG Flows · $c$-functions from the Null Energy Condition · 0.92
Compares with it 3 papers
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Furthermore, we will find that the beta function associated to the dimensionless coupling, $g_L = L^d-Δ$, is proportional to the derivative of the prepotential, $W'$, as opposed to the usual holographic beta function $W'/W$ [ref] .
Dimensional regularization for holographic RG flows · Introduction · 0.97
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Notice that this analysis is equivalent to that of [ref] , provided that we identify the central charge function as $c(z) ∼ (T_zz)^-5/2$.
A new 6d fixed point from holography · Introduction · 0.85
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Thus there is less sensitivity to the bulk geometry is the present construction of a holographic c-theorem using the entanglement entropy than in the original discussions [ref] .
Comments on Holographic Entanglement Entropy and RG Flows · Discussion · 0.87
Cites it as support 1 paper
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Indeed, the $κ_hol$ in the holographic model decreases under any RG flow thanks to the holographic $c$-theorem [ref] that provides the constraint $L_UV ≥L_IR$ for the AdS radii in the UV and IR fixed points.
Entanglement Entropy of Annulus in Three Dimensions · Universal behaviors · 0.98
Cites it as background 49 papers
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Considerable progress on constructing $c$-functions has been made from the holographic perspective: Various holographic $c$-theorems have been established in this context by making use of the Null Energy Condition (NEC) [ref] , as well as using the entanglement entropy perspective to analyze holographic RG flows [ref] .
$c$-functions in Higher-derivative Flows Across Dimensions · Introduction and summary · 0.93
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For the classical renormalization group flows, [ref] established a c-theorem, demonstrating that so long as the bulk geometry satisfied a suitable energy condition, the c-function of [ref] would be monotonically decreasing along the flow from the UV to the IR (see also [ref] ).
Reversing Renormalization-Group Flows with AdS/CFT · Introduction · 0.90
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Here we begin with a review of the holographic c-theorem as originally studied by [ref] for Einstein gravity.
Comments on Holographic Entanglement Entropy and RG Flows · Review of holographic c-theorems · 0.99
Discussion
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