REVIEW
UV/IR Relations in AdS Dynamics
High Energy Physics - Theory · Submitted 3 Sep 1998 · 24 references
Pith's verdict: A clean, honest clarification note that separates the holographic and stretched-string UV/IR maps; the p=6 section is the only place it asserts more than it shows.
Why Pith says this
Highlight any text to comment on it.
Referee report
The paper
The paper claims
The AdS/CFT correspondence has been used with two different energy–distance relations, and this paper shows they agree only in conformal backgrounds: for nonconformal Dp-brane throats they differ in functional form, which changes which of a
The reading
What carries the argument
The load-bearing device is the wave equation for a massless scalar of angular momentum $ell$ minimally coupled to the Einstein-frame Dp metric, Eq. (2.14). Its two competing terms — the angular barrier going as $U^{-2}$ and the momentum term $k^2 g^2_{YM} N U^{7-p}$ — balance at a radius that defines the holographic energy–radius map, and this same 'all metric terms scale together' criterion reproduces the conformal results and the black-hole temperature/radius relation. The competing map is the stretched-string energy: the world-sheet measure cancels the string tension so that the energy equals the coordinate length $U$ for a D3 probe, generalizing to $tau = U^2$ for an M2-brane ending on an M5-brane. Comparing the two maps through the effective coupling is what produces the case analysis by $p$.
Extended reading notes
Core claim
The central claim is that 'the AdS/CFT distance–energy relation' is not one thing. The holographic relation, read off from the scaling of the minimally coupled scalar wave equation (equivalently, from requiring that the two terms of the metric share a common scaling), gives $E = U^{(5-p)/2}/(g_{YM}N^{1/2})$ for a Dp-brane throat, while a stretched string ending on a probe brane gives $E = U$. For $p=3$ these coincide up to normalization; for other $p$ they do not, and the effective gauge coupling $g^2_{eff} = g^2_{YM} N E^{p-3}$ therefore runs differently depending on which probe is doing the measuring. The authors show that for $p le 4$ the weak-coupling conditions agree for both probes, so the existing catalogue of effective descriptions survives; at $p=5$ the holographic relation degenerates and the boundary theory loses renormalized local operators, the field spread growing as $g_{YM}N^{1/2}ln(U_0/U)$; at $p=6$ the supergravity probe's radius decreases with energy, giving a gauge theory near the origin and a supergravity theory far away that are isolated from one another. They also check that the holographic entropy formula reproduces the nonextremal Dp-brane entropy at temperature $T=E$.
Load-bearing premise
The whole case analysis rests on taking the radius at which the two terms of the scalar wave equation balance — equivalently, where all terms in the metric scale alike — as the definition of the holographic energy–radius map; if the relevant localization scale were set by something else, such as the full Green's function rather than the scaling of the wave operator, the functional forms in Eq. (2.15) and the weak-coupling comparisons built on them would change.
Editorial extensions
If this is right
- For $p le 4$ the earlier effective-description catalogue stands for both kinds of probe, because $g^2_{eff} ll 1$ holds for both at the same radii.
- For $p=5$ holography fails sharply: boundary data must scale as $U^{(g^2_{YM}Nk^2)^{1/2}}$ to give a finite result, which has no Fourier transform, so renormalized local operators do not exist.
- For $p=6$ the apparent paradox of two weakly coupled descriptions at once is resolved by isolation: the gauge theory sits at $U^3 < g_{YM}^{-2}N^{-1}$ and the supergravity at $U^3 > g_{YM}^{-2}N^{-1}$, with no overlap.
- The holographic entropy $S = L^p E^{(9-p)/(5-p)} N^2 [g^2_{YM}N]^{(p-3)/(5-p)}$ matches the nonextremal Dp-brane entropy at $T=E$, extending the D3 result to all $p$.
- For $p=1$ the apparent gap left by the brane-probe relation is not a real gap, because at those scales the D-string probe is replaced by an $ilde F$-string description and the scale $E=U$ loses its meaning.
Reading between the lines
- The distinction suggests a general diagnostic: whenever a duality map is used to compare weak-coupling regimes, one should check whether both sides are using the same probe type, since the two maps agree only when the background is conformal.
- The $p=5$ loss of local operators looks like a clean example of a holographic dual that exists in momentum space but not in position space; it would be worth asking whether that momentum-space theory is still local in any weaker sense.
- The $p=6$ isolation argument implies that 'two weakly coupled descriptions of one system' is not by itself a contradiction provided the sectors decouple, a criterion that could be applied to other suspected duality paradoxes.
- If the holographic map is the one governing thermodynamics, then the brane-probe energy $E=U$ is best read as a self-energy scale rather than a cutoff, matching the interpretation of the stretched string as a heavy external charge.
Original abstract
We point out that two distinct distance--energy relations have been discussed in the AdS/CFT correspondence. In conformal backgrounds they differ only in normalization, but in nonconformal backgrounds they differ in functional form. We discuss the relation to probe processes, the holographic principle, and black hole entropies.
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 point out that two distinct distance--energy relations have been discussed in the AdS/CFT correspondence. In conformal backgrounds they differ only in normalization, but in nonconformal backgrounds they differ in functional form. We discuss the relation to probe processes, the holographic principle, and black hole entropies.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We point out that two distinct distance--energy relations have been discussed in the AdS/CFT correspondence. | background 0.54 | 0.45 | 0.13 | asserted 1.00 |
| s1 | In conformal backgrounds they differ only in normalization, but in nonconformal backgrounds they differ in functional form. | result 0.73 | 0.17 | 0.30 | asserted 1.00 |
| s2 | We discuss the relation to probe processes, the holographic principle, and black hole entropies. | contribution 0.98 | 0.77 | 0.12 | asserted 0.56 |
What was examined, and what was not
- arXiv listing abstract v2
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
References
How later papers used it
90 later papers cite it
2 later papers by other authors are listed below: 1 used its method or tool and 1 cited it as support.
Uses its method or tool 1 of 2 papers with this label
-
Followed this paper by considering the s-wave mode of a massless scalar field on the background.
Gravitational solitons and non-relativistic string theory (2025) · 0.85 · paraphrased: the licence does not allow quoting
Cites it as support 1 of 3 papers with this label
-
Said its result is consistent with this paper's expectation that particle wave-functions are localized in the supergravity regime around the radial position corresponding to their compositeness scale.
Metastable Vacua in Warped Throats at Non-Isolated Singularities (2010) · 0.97 · paraphrased: the licence does not allow quoting
How the literature uses it
86 arXiv papers cite this in 109 sentences
Papers citing it · 80 sentences without a confident label
Uses its method or tool 2 papers
-
Nevertheless it is possible to use the results in [ref] to evaluate the on-shell action of the spherical brane solutions and reproduce the scaling of the free energy with $N$ and $λ_eff$ in [ref].
Spherical Branes · Introduction · 0.95
-
Indeed, following [ref] one considers the s-wave mode of a massless scalar field on the background [ref].
Gravitational solitons and non-relativistic string theory · Regime of validity of the near-horizon fundamental string soliton · 0.85
Cites it as support 3 papers
-
This is in line with the prediction by Peet and Polchinski that there are two distinct phases for SYM in seven dimensions, one of them being gravitational [ref] .
Seven-dimensional super Yang-Mills at negative coupling · Introduction and summary · 0.97
-
The salient feature which establishes this interpretation is that the Wightman functions of LSTs can be shown to have the exponential growth characterstic of the Hagedorn density of states [ref] .
UV properties of Galileons: Spectral Densities · The case of Little String Theory · 0.98
-
Happily, this is consistent with the expectation that particle wave-functions are localized in the supergravity regime around the radial position corresponding to their compositeness scale [ref] .
Metastable Vacua in Warped Throats at Non-Isolated Singularities · Cascade · 0.97
Cites it as background 24 papers
-
This goes by the name “Domain Wall/QFT correspondence" [ref] .[Henceforth labeled “DW/QFT" for short.] The fact that the metric ([ref]) is conformal to AdS can be phrased as crucial to the duality, which was established by decoupling the near-horizon dynamics of non-conformal D-branes: passage to a conformal, so-called “dual" frame in which the D-brane near-horizon metric becomes AdS$_p+2×S^8-p$ reveals a manifest $(p+2)$-dimensional gravitational description, in which we identify the radial direction with the energy scale of the dual field theory [ref] .
Domain Wall Holography for Finite Temperature Scaling Solutions · Introduction and summary · 0.90
-
For systems with a gravity dual, the AdS/CFT correspondence [ref] provides a striking geometric picture for the renormalization group flow and the resulting low energy behavior; the radial direction in the bulk can be associated with the energy scale of the boundary theory [ref] , and the radial flow in the bulk geometry can be interpreted as the renormalization group flow of the boundary theory [ref] .
Integrating out geometry: Holographic Wilsonian RG and the membrane paradigm · Introduction · 0.97
-
In the context of AdS/CFT, there are two existing approaches: Wilson-like holographic RG [ref] and the Jaynes maximization of entropy subject to contraints [ref] .
Losing the IR: a Holographic Framework for Area Theorems · Introduction · 0.95
Discussion
Disagree with the review, or know something it missed? Leave a comment, highlight any passage above to comment on it, or challenge this review formally.