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Froissart bound for/from CFT Mellin amplitudes
by Parthiv Haldar, Aninda Sinha
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Submission summary
| Authors (as registered SciPost users): | Parthiv Haldar · Aninda Sinha |
| Submission information | |
|---|---|
| Preprint Link: | scipost_202004_00044v1 (pdf) |
| Date submitted: | 2020-04-03 02:00 |
| Submitted by: | Haldar, Parthiv |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
We derive bounds analogous to the Froissart bound for the absorptive part of CFT$_d$ Mellin amplitudes. Invoking the AdS/CFT correspondence, these amplitudes correspond to scattering in AdS$_{d+1}$. We can take a flat space limit of the corresponding bound. We find the standard Froissart-Martin bound, including the coefficient in front for $d+1=4$ being $\pi/\mu^2$, $\mu$ being the mass of the lightest exchange. For $d>4$, the form is different. We show that while for $CFT_{d\leq 6}$, the number of subtractions needed to write a dispersion relation for the Mellin amplitude is equal to 2, for $CFT_{d>6}$ the number of subtractions needed is greater than 2 and goes to infinity as $d$ goes to infinity.
Current status:
Reports on this Submission
Report #2 by Matthew Dodelson (Referee 2) on 2020-5-6 (Invited Report)
- Cite as: Matthew Dodelson, Report on arXiv:scipost_202004_00044v1, delivered 2020-05-05, doi: 10.21468/SciPost.Report.1664
Report
This paper initiates the program of generalizing the Froissart bound to holographic conformal field theories in the flat space limit. The Mellin amplitude in conformal field theory plays the role of the scattering amplitude in ordinary quantum field theory, and the bounds derived in this paper are on the imaginary part of the Mellin amplitude. Just like in the flat space case, the authors use the assumption of polynomial boundedness to derive their bounds. Both the forward and nonforward limits are discussed.
This is an important and original paper, and I strongly suggest its publication.
Requested changes
1. The authors state that the flat space limit involves taking R/l_planck large. I believe that one also requires the dimensionless quantity R/l_string to be large.
2. In equation (3.26), the upper bound of the integral at infinity is omitted.
3. Some minor spelling errors: on page 3, unitarty should be unitarity. On page 4, analytitcity should be analyticity. On page 5, indepnpendent should be independent. On page 7, prcatical should be practical. On page 13, puting should be putting. On page 15, depepndency should be dependency. On page 20, hyperegometric should be hypergeometric.
Report #1 by Connor Behan (Referee 1) on 2020-5-3 (Invited Report)
- Cite as: Connor Behan, Report on arXiv:scipost_202004_00044v1, delivered 2020-05-03, doi: 10.21468/SciPost.Report.1654
Strengths
1. Interesting result with connections to collider experiments.
2. Starts off with two helpful overviews, one for each side of the correspondence.
3. Excellent use of appendices to make section 4 flow nicely.
4. Provides a great demonstration of the progress that can be gained by combining old and new work on the S-matrix.
Weaknesses
1. There are a few typos discussed below.
2. "Flat-space" vs "flat space", $\Gamma^2(x)$ vs $\Gamma(x)^2$ and $u$ vs $\hat{u}$ are not consistent.
3. Some of the limits being used are more rigorous than others.
Report
This article presents a new method for bounding the absorptive part of a massive scattering amplitude. Instead of working in flat space, the authors take the background to be a nearly flat AdS space which allows them to exploit the duality with a CT (nonlocal CFT) in one lower dimension. This alone would already make for an interesting paper. However, the final result contains some surprises compared to the usual Froissart bound. Specifically, it is stronger for (bulk) dimension d < 4. Even for d = 4, when the bound has the same form, the authors find the remarkable fact that the exchanged mass can be replaced with the external mass yielding a better fit to experimental data. Apparently, after assuming polynomial boundedness in s for some ellipse, t can be deformed to a more forgiving value in this formulation.
Since the paper is highly technical, there are a few steps that could benefit from more explanation. First, why does the $\sin^2$ disappear after (4.14)? Second, the discussion around (4.3) says $\Delta_\phi \gg 1, \tau \gg 1$ but it should also say they are of the same order. Was the sum (4.19), which supports this relation between $\Delta_\phi$ and $\tau$, found by assuming it in the first place? If so, there should be some argument about why it is safe to take this limit self-consistently. Third, it would be nice to read more about which part of the outer sum dominates in (4.37). It starts from zero but various assumptions about the spin being large are used inside the sum.
My other requests are just about typos. SciPost should look forward to publishing the final version.
Requested changes
1. Update the reference to appendix E on page 8 so that is says appendix G.
2. Footnote 5 should probably say "which will make a difference".
3. Appendix A says "for" instead of "form" and appendix D says "This" instead of "this".
4. The line under (E.1) should say "able to approximate this sum" or something similar.
5. Sentences that would sound better with articles are "there exists A certain" on page 5 and "obtaining AN asymptotic upper bound" on page 15.
6. The sentence under (3.2) should say there are $n(n-3)/2$ independent variables because the specialization to 4 points is only made in the next sentence.
7. There appears to be a missing division sign in (B.4), a $45m^2$ in (C.9) and unmatched parentheses in (D.7).
8. It is not obvious that the flat space limit would lead to $\tau \sim \Delta_\phi$ and $\ell \gg 1$. If it is possible to eliminate all doubts about this, that should be done in section 4.1.