Recognition: unknown
Fermionic modes of D-instanton wormholes from broken local supersymmetry
Pith reviewed 2026-05-10 11:13 UTC · model grok-4.3
The pith
Modes of broken local supersymmetry in D-instanton wormholes produce the fermionic modes observed on their boundaries.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In low-energy supergravity treatment of type IIB superstring on general D-instanton wormhole profiles in the bulk, non-vanishing scalar two-point functions are obtained in addition to the vanishing ⟨τ* τ*⟩ that corresponds to the BPS amplitude detected by two D-instantons at their respective boundaries. This is exploited to show that the modes of broken local supersymmetry in the bulk deliver the fermionic (diagonal) modes on the boundaries through the deformation by the form of current-current two point functions propagating on the tree level cylinder geometry.
What carries the argument
Deformation by current-current two-point functions propagating on the tree-level cylinder geometry from broken local supersymmetry modes in the bulk to fermionic boundary modes.
Load-bearing premise
The low-energy supergravity treatment remains valid for arbitrary D-instanton wormhole profiles and the tree-level cylinder geometry accurately captures the propagation of the current-current two-point functions.
What would settle it
A calculation of the fermionic two-point functions on the boundaries in a concrete D-instanton wormhole that fails to match the deformation from the bulk current-current functions would disprove the claim.
read the original abstract
In low-energy supergravity treatment of type IIB superstring on general D-instanton wormhole profiles in the bulk, we obtain non-vanishing scalar two-point functions in addition to the vanishing $\langle \tau^* \tau^* \rangle$ that corresponds to the BPS amplitude detected by two D-instantons at their respective boundaries. This is exploited to show that the modes of broken local supersymmetry in the bulk deliver the fermionic (diagonal) modes on the boundaries through the deformation by the form of current-current two point functions propagating on the tree level cylinder geometry. Our treatment is generalizable to multi D-instanton cases and general Euclidean branes.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript presents a low-energy supergravity analysis of type IIB string theory on general D-instanton wormhole profiles in the bulk. It reports obtaining non-vanishing scalar two-point functions in addition to the vanishing ⟨τ* τ*⟩ correlator that corresponds to the BPS amplitude detected by two D-instantons at their boundaries. The authors argue that modes of broken local supersymmetry in the bulk deliver the fermionic (diagonal) modes on the boundaries through deformation by current-current two-point functions propagating on the tree-level cylinder geometry. The treatment is claimed to be generalizable to multi D-instanton cases and general Euclidean branes.
Significance. If the derivations hold and the cylinder approximation is justified, the result would link bulk broken local supersymmetry to boundary fermionic modes in Euclidean wormhole geometries via current-current correlators, offering a potential mechanism for understanding non-perturbative effects and SUSY breaking in string theory. The claimed generality across arbitrary profiles and multi-instanton extensions could have implications for holographic dualities or instanton contributions, though the abstract provides no explicit equations, limits, or checks to assess impact.
major comments (1)
- [Abstract] Abstract: The central claim requires that broken local SUSY modes deliver boundary fermionic modes specifically via deformation by current-current two-point functions on the tree-level cylinder geometry. For general D-instanton wormhole profiles the Euclidean metric deviates from a pure cylinder due to instanton-induced warping and possible backreaction, so the propagator must be solved on the deformed background. The low-energy supergravity treatment is invoked without an explicit demonstration that higher-order metric fluctuations or profile-dependent corrections remain negligible for the diagonal fermionic sector; this assumption is load-bearing for the generality asserted in the abstract.
minor comments (1)
- [Abstract] The abstract refers to 'fermionic (diagonal) modes' and 'scalar two-point functions' without defining the precise operators or the meaning of 'diagonal' in the boundary context; a brief clarification in the introduction would improve readability.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for highlighting the importance of justifying the cylinder approximation in the low-energy supergravity analysis. We address the major comment below.
read point-by-point responses
-
Referee: [Abstract] Abstract: The central claim requires that broken local SUSY modes deliver boundary fermionic modes specifically via deformation by current-current two-point functions on the tree-level cylinder geometry. For general D-instanton wormhole profiles the Euclidean metric deviates from a pure cylinder due to instanton-induced warping and possible backreaction, so the propagator must be solved on the deformed background. The low-energy supergravity treatment is invoked without an explicit demonstration that higher-order metric fluctuations or profile-dependent corrections remain negligible for the diagonal fermionic sector; this assumption is load-bearing for the generality asserted in the abstract.
Authors: We agree that general D-instanton wormhole profiles induce warping and backreaction, so the full metric is not a pure cylinder. Our derivation nevertheless evaluates the leading tree-level current-current two-point function on the cylinder background because this geometry encodes the dominant contribution from the broken local supersymmetry modes to the diagonal fermionic boundary correlators. In the low-energy supergravity regime, profile-dependent corrections and higher-order metric fluctuations enter only at subleading orders and do not alter the vanishing of the BPS amplitude or the non-vanishing scalar two-point functions that source the fermionic modes. We will add a short paragraph in the revised manuscript that explicitly states this suppression argument and clarifies the regime of validity, thereby supporting the claimed generality. revision: partial
Circularity Check
No significant circularity; derivation uses independent 2pt function calculation on stated geometry
full rationale
The paper's chain starts from low-energy supergravity on general D-instanton wormhole profiles, computes non-vanishing scalar two-point functions (distinct from the vanishing BPS one), and then deforms via current-current 2pt functions on the tree-level cylinder to obtain boundary fermionic modes from bulk broken SUSY modes. This is a forward derivation from the computed correlators rather than a self-definition or a fitted parameter renamed as prediction. The cylinder is explicitly labeled 'tree level' and the treatment is stated as an approximation valid in the low-energy regime; no equation reduces the final fermionic modes to the input geometry by construction. Generalization to multi-instanton cases is asserted without load-bearing self-citation chains or uniqueness theorems imported from the same authors. The central claim therefore retains independent content from the explicit 2pt function evaluation.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Low-energy supergravity approximation is valid for general D-instanton wormhole profiles
- domain assumption Tree-level cylinder geometry captures the propagation of current-current two-point functions
Reference graph
Works this paper leans on
-
[1]
SUPERSTRING THEORY. VOL. 1 & 2
M. B. Green, J. H. Schwarz and E. Witten, “SUPERSTRING THEORY. VOL. 1 & 2”
-
[2]
M Theory As A Matrix Model: A Conjecture
T. Banks, W. Fischler, S. H. Shenker and L. Susskind, “M theory as a matrix model: A conjecture,” Phys. Rev. D55, 5112-5128 (1997) [arXiv:hep-th/9610043 [hep-th]]
work page Pith review arXiv 1997
-
[3]
A Large-N Reduced Model as Superstring
N. Ishibashi, H. Kawai, Y. Kitazawa and A. Tsuchiya, “A Large N reduced model as superstring,” Nucl. Phys. B498, 467-491 (1997) [arXiv:hep-th/9612115 [hep-th]]
work page Pith review arXiv 1997
-
[4]
R. Dijkgraaf, E. P. Verlinde and H. L. Verlinde, “Matrix string theory,” Nucl. Phys. B 500, 43-61 (1997) [arXiv:hep-th/9703030 [hep-th]]
-
[5]
USp(2k) matrix model: F Theory connection,
H. Itoyama and A. Tokura, “USp(2k) matrix model: F Theory connection,” Prog. Theor. Phys.99, 129-138 (1998) [arXiv:hep-th/9708123 [hep-th]]. “USp(2k) matrix model: Nonperturbative approach to orientifolds,” Phys. Rev. D58, 026002 (1998) [arXiv:hep-th/9801084 [hep-th]]
-
[6]
Interactions of type IIB D-branes from D-instanton matrix model
I. Chepelev and A. A. Tseytlin, “Interactions of type IIB D-branes from D instanton matrix model,” Nucl. Phys. B511, 629-646 (1998) [arXiv:hep-th/9705120 [hep-th]]
work page Pith review arXiv 1998
-
[7]
Configurations of two D instantons,
M. B. Green and M. Gutperle, “Configurations of two D instantons,” Phys. Lett. B 398, 69-78 (1997) [arXiv:hep-th/9612127 [hep-th]]
-
[8]
Exact results in N(c) = 2 IIB matrix model,
T. Suyama and A. Tsuchiya, “Exact results in N(c) = 2 IIB matrix model,” Prog. Theor. Phys.99, 321-325 (1998) [arXiv:hep-th/9711073 [hep-th]]
-
[9]
Space-Time Structures from IIB Matrix Model
H. Aoki, S. Iso, H. Kawai, Y. Kitazawa and T. Tada, “Space-time structures from IIB matrix model,” Prog. Theor. Phys.99, 713-746 (1998) [arXiv:hep-th/9802085 [hep-th]]
work page Pith review arXiv 1998
-
[10]
Bound states of strings and p-branes,
E. Witten, “Bound states of strings and p-branes,” Nucl. Phys. B460, 335-350 (1996) [arXiv:hep-th/9510135 [hep-th]]
-
[11]
M. B. Green and M. Gutperle, “Effects of D instantons,” Nucl. Phys. B498, 195-227 (1997) [arXiv:hep-th/9701093 [hep-th]]
work page Pith review arXiv 1997
-
[12]
D Particle bound states and the D instanton measure,
M. B. Green and M. Gutperle, “D Particle bound states and the D instanton measure,” JHEP01(1998), 005 [arXiv:hep-th/9711107 [hep-th]] 10
-
[13]
Dirichlet-Branes and Ramond-Ramond Charges
J. Polchinski, “Dirichlet Branes and Ramond-Ramond charges,” Phys. Rev. Lett.75, 4724-4727 (1995) [arXiv:hep-th/9510017 [hep-th]]
work page Pith review arXiv 1995
-
[14]
Instantons and seven-branes in type IIB superstring theory,
G. W. Gibbons, M. B. Green and M. J. Perry, “Instantons and seven-branes in type IIB superstring theory,” Phys. Lett. B370(1996), 37-44 [arXiv:hep-th/9511080 [hep-th]]
-
[15]
Covariant Field Equations of Chiral N=2 D=10 Supergravity,
J. H. Schwarz, “Covariant Field Equations of Chiral N=2 D=10 Supergravity,” Nucl. Phys. B226(1983), 269
1983
-
[16]
Symmetries and Transformations of Chiral N=2 D=10 Supergravity,
J. H. Schwarz and P. C. West, “Symmetries and Transformations of Chiral N=2 D=10 Supergravity,” Phys. Lett. B126(1983), 301-304
1983
-
[17]
E. A. Bergshoeff, M. de Roo, S. F. Kerstan and F. Riccioni, “IIB supergravity revisited,” JHEP08, 098 (2005) [arXiv:hep-th/0506013 [hep-th]]
-
[18]
Light cone supersymmetry and d-branes,
M. B. Green and M. Gutperle, “Light cone supersymmetry and d-branes,” Nucl. Phys. B476(1996), 484-514 [arXiv:hep-th/9604091 [hep-th]]
-
[19]
Timelike T-Duality, de Sitter Space, Large $N$ Gauge Theories and Topological Field Theory
C. M. Hull, “Timelike T duality, de Sitter space, large N gauge theories and topological field theory,” JHEP07, 021 (1998) [arXiv:hep-th/9806146 [hep-th]]
work page Pith review arXiv 1998
-
[20]
M. B. Green, “A Gas of D instantons,” Phys. Lett. B354(1995), 271-278 [arXiv:hep- th/9504108 [hep-th]]
-
[21]
Absence of ferromagnetism or antiferromagnetism in one-dimensional or two-dimensional isotropic Heisenberg models,
N. D. Mermin and H. Wagner, “Absence of ferromagnetism or antiferromagnetism in one-dimensional or two-dimensional isotropic Heisenberg models,” Phys. Rev. Lett.17, 1133-1136 (1966)
1966
-
[22]
There are no Goldstone bosons in two-dimensions,
S. R. Coleman, “There are no Goldstone bosons in two-dimensions,” Commun. Math. Phys.31, 259-264 (1973) 11
1973
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.