REVIEW
Non-Perturbative Superpotentials In String Theory
High Energy Physics - Theory · Submitted 5 Apr 1996 · 26 references
Pith's verdict: The χ(D,O_D)=1 selection rule is the real contribution and it holds up; the paper is a vanishing criterion plus a leading exponential, not the full superpotential the abstract advertises.
T0 · AI review
Why Pith says this
Highlight any text to comment on it.
Referee report
The paper
The paper claims
A five-brane wrapped on a divisor D generates a superpotential only if the arithmetic genus of D is exactly one, giving a computable yes-or-no test for supersymmetry breaking in M-theory, F-theory, and heterotic compactifications.
The reading
Extended reading notes
Core claim
A five-brane wrapped on a complex divisor D of a Calabi-Yau four-fold generates a superpotential if and only if chi(D, O_D) = 1, where chi(D, O_D) = sum (-1)^n h^n(D) is the arithmetic genus. Witten states it as: 'a superpotential can only be generated by wrapping a five-brane on D if chi(D, O_D) = 1', with the partial converse that any divisor with h^1 = h^2 = h^3 = 0 does contribute. Because chi depends only on the cohomology class of D (Eq. 2.9), the test is computable from topological data, and it transfers to F-theory and heterotic compactifications.
Load-bearing premise
In section 2, immediately after introducing the SO(2) normal-bundle generator W whose anomaly controls the whole argument, Witten writes that 'it is somewhat hard to answer this question definitively because the five-brane action is not fully known', and then: 'At any rate, this assumption will be made in the present paper.' The assumption is that W is an exact symmetry of the five-brane world-volume action, meaning no W-violating couplings such as psi-psi-R exist. If W is not exact, the anomaly matching that fixes the W charge of e^{-(V_D + i phi_D)}, and hence the chi = 1 criterion, does not go through.
Original abstract
The non-perturbative superpotential can be effectively calculated in $M$-theory compactification to three dimensions on a Calabi-Yau four-fold $X$. For certain $X$, the superpotential is identically zero, while for other $X$, a non-perturbative superpotential is generated. Using $F$-theory, these results carry over to certain Type IIB and heterotic string compactifications to four dimensions with $N=1$ supersymmetry. In the heterotic string case, the non-perturbative superpotential can be interpreted as coming from space-time and world-sheet instantons; in many simple cases contributions come only from finitely many values of the instanton numbers.
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
The non-perturbative superpotential can be effectively calculated in $M$-theory compactification to three dimensions on a Calabi-Yau four-fold $X$. For certain $X$, the superpotential is identically zero, while for other $X$, a non-perturbative superpotential is generated. Using $F$-theory, these results carry over to certain Type IIB and heterotic string compactifications to four dimensions with $N=1$ supersymmetry. In the heterotic string case, the non-perturbative superpotential can be interpreted as coming from space-time and world-sheet instantons; in many simple cases contributions come only from finitely many values of the instanton numbers.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The non-perturbative superpotential can be effectively calculated in $M$-theory compactification to three dimensions on a Calabi-Yau four-fold $X$. | contribution 0.33 | 0.35 | 0.27 | asserted 0.83 |
| s1 | For certain $X$, the superpotential is identically zero, while for other $X$, a non-perturbative superpotential is generated. | result 1.00 | 0.51 | 0.29 | asserted 1.00 |
| s2 | Using $F$-theory, these results carry over to certain Type IIB and heterotic string compactifications to four dimensions with $N=1$ supersymmetry. | result 0.48 | 0.46 | 0.22 | asserted 0.93 |
| s3 | In the heterotic string case, the non-perturbative superpotential can be interpreted as coming from space-time and world-sheet instantons; in many simple cases contributions come only from finitely many values of the instanton numbers. | interpretation 0.99 | 0.52 | 0.17 | asserted 0.73 |
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 the literature uses it
209 arXiv papers cite this in 356 sentences
Papers citing it · 257 sentences without a confident label
Contests it 1 paper
-
The number of zero modes is determined by the geometry of $π^*(D)$ [ref] and divisors with the right of zero modes to contribute to the superpotential are known as rigid.[The condition given in [ref] on the geometry of $π^*(D)$ to give two zero modes is in fact neither necessary nor sufficient due to the effects of fluxes and spacetime-filling D3/M2-branes on the zero mode spectrum [ref] ]
Towards the Non-Perturbative Completion of 4d N=1 Effective Theories of Gravity · Beyond Supersymmetry Enhancement · contest 0.78
Builds on it 4 papers
-
As a consequence, a divisor $D$ with star-crossing singularities contributes to the superpotential in a particular Calabi-Yau if there exists a birationally-equivalent geometry in which the image of $D$ is smooth and fulfills the condition of [ref] .
Superpotentials from Singular Divisors · Conclusions · 0.91
-
It should however be possible to extend the analysis of [ref] to such warped cases.
The AdS/CFT Correspondence and Symmetry Breaking · Non-perturbative superpotentials · 0.95
-
Clearly this goes beyond the analysis in [ref] , since one would require a suitable generalization to M5-brane instantons on singular 6-cycles.
Non-perturbative superpotentials across lines of marginal stability · Topology changing transitions in F-theory · 0.91
Uses its method or tool 2 papers
-
For a given geometry, one may, in principle, determine which four-cycles $Σ^a$ support Euclidean D3-brane superpotential terms — and so, using [ref], compute the axion charge matrix $𝒬_a^ i$ — by counting the zero modes of suitable Dirac operators on the cycles $Σ^a$ [ref] .
Superradiance in String Theory · Instanton potential · 0.86
-
To compute such contributions one should perform the path-integral over all bosonic and fermionic fields [ref] and include also the contribution of the incoming M2-branes as in [ref] .
Hidden Selection Rules, M5-instantons and Fluxes in F-theory · M5-action and M2-insertions · 0.86
Compares with it 2 papers
-
This parallels the situation for the partition function of M5-instantons in M/F-theory [ref] .
On Fluxed Instantons and Moduli Stabilisation in IIB Orientifolds and F-theory · Fluxed instantons in supergravity · 0.97
-
However, at this point we should recall that the situation in [ref] is slightly different from the one at hand.
Baryonic symmetries and M5 branes in the AdS_4/CFT_3 correspondence · Non-perturbative superpotentials from six-cycles · 0.80
Cites it as background 80 papers
-
For the case of Euclidean D3-branes wrapping a smooth effective divisor $D$, Witten presented a counting of fermion zero modes in terms of the cohomology of the structure sheaf $𝒪_D$, and identified a sufficient condition for a superpotential contribution [ref] .
Superpotentials from Singular Divisors · Conclusions · 0.81
-
The third step, since $h^1,1=1$, is to introduce the universal Kähler modulus $T$ with the known Kähler potential $K_T$, as well as the associated non-perturbative “worldsheet” instanton superpotential $W_T$ [ref] .
Stable Vacua with Realistic Phenomenology and Cosmology in Heterotic M-theory Satisfying Swampland Conjectures · Deriving the potential energy · 0.84
-
Standard LVS: The LVS scheme of moduli stabilisation considers a combination of perturbative $(α^')^3$ corrections to $K$ [ref] and a non-perturbative contribution to $W$ [ref] .
Global Embedding of Fibre Inflation in Perturbative LVS · LVS schemes of moduli stabilisation · 0.99
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.