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Supersymmetry for Gauged Double Field Theory and Generalised Scherk-Schwarz Reductions

High Energy Physics - Theory · Submitted 13 May 2013 · 69 references

Pith's verdict: A genuine fermionic completion of gauged DFT with a plausible but under-displayed equivalence argument at its core.

T0 · AI review

How this review was made: An AI referee (selfhosted/deepseek-v4.1-flash) read the paper on November 10, 2026 and answered a fixed list of questions about it. T0 is the starting level every paper gets. The levels describe how deeply Pith has checked the paper, never the authors.

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  5. T4 Proof Those claims proved, and the proof checked by computer.

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arXiv ID1305.2747 (version 2)
Pith IDWTATH4WK, Pith's permanent record of this paper and its review
CitationDavid S. Berman, Kanghoon Lee. "Supersymmetry for Gauged Double Field Theory and Generalised Scherk-Schwarz Reductions." arXiv:1305.2747 (2013). https://pith.science/paper/WTATH4WK
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Referee report
The paper

The paper claims

Supersymmetry in double field theory survives when the strong constraint is relaxed, provided the extra coordinate dependence is of generalised Scherk-Schwarz type, and the reduced theory has the same Killing spinor equations as the gauged

The reading

Double field theory makes the $O(D,D)$ T-duality symmetry of string theory manifest by doubling the coordinates, but it has usually required a strong constraint (the section condition) that removes dependence on the extra coordinates. Earlier supersymmetric versions of the theory relied on that constraint, which suggested that relaxing it would break supersymmetry. Berman and Lee argue the opposite: once the extra coordinate dependence is restricted to a generalised Scherk-Schwarz factorisation, the theory still has a supersymmetric action, explicit supersymmetry variations, and a well-defined fermionic sector. They then compare this reduced theory with the gauged version of double field theory and claim the two have identical Killing spinor equations, so the extra dual coordinates can be treated as physical without destroying supersymmetry.

What carries the argument

The load-bearing device is the semi-covariant derivative $nabla_M$ built with a connection $Gamma^P{}_{MN}$ that is $O(D,D)$-compatible, metric-compatible with respect to the two projectors $P_{MN}=tfrac12(J_{MN}+H_{MN})$ and $bar P_{MN}=tfrac12(J_{MN}-H_{MN})$, and torsion-free only up to a gauge transformation, $Gamma_{[MNP]}=tfrac13 f_{MNP}$, where $f_{MNP}$ are the structure constants of the gauged theory. Individual derivatives are not fully covariant under twisted generalised Lie derivatives, but contracting them with the rank-six projection operators $P^{P M N}{}_{QRS}$ and $bar P^{P M N}{}_{QRS}$ produces fully covariant objects, and it is this projection step that lets the authors assemble the curvature scalars and the spin connections into a supersymmetric action.

Extended reading notes

Core claim

The paper constructs a half-maximal supersymmetric gauged double field theory whose bosonic sector is the DFT-dilaton and the pair of double vielbeins and whose fermionic sector is a gravitino and a dilatino, with action $L=e^{-2d}[2P^{MP}P^{NQ}S_{MN PQ}+4i(bar{rho}gamma^m D_m rho - 2 bar{psi}^{bar m}D_{bar m}rho - bar{psi}^{bar m}gamma^m D_m psi^{bar m})]$ built from the semi-covariant curvature and the gauged Dirac operators. The authors state that this action is invariant, to leading order in fermions, under the variations $delta d = -tfrac{i}{12}bar{epsilon}rho$, $delta V^{Mm} = -i bar{V}^{Mbar q}bar{epsilon}gamma^m psi^{bar q}$, $delta rho = -gamma^m D_m epsilon$, $delta psi^{bar m} = D^{bar m}epsilon$. The second claim is a comparison: the generalised Scherk-Schwarz reduction of the parent ungauged theory produces a connection that differs from the gauged connection by a term involving the twist matrix, and the corresponding spin connections differ by the projected quantity in their equation (4.10); the authors assert that this difference vanishes when contracted into the semi-covariant derivatives, so the Killing spinor equations of the gauged and the Scherk-Schwarz reduced theories coincide exactly.

Load-bearing premise

The claim that the gauged and Scherk-Schwarz reduced theories have identical Killing spinor equations rests on the assertion that the difference of spin connections in equation (4.10) vanishes once contracted with the projection operators, a cancellation the paper states rather than demonstrating term by term.

Editorial extensions

If this is right

  • Supersymmetric double field theory does not need the strong constraint: Scherk-Schwarz factorisation is enough to keep the supersymmetry variations consistent.
  • The gauged double field theory and the generalised Scherk-Schwarz reduced theory share the same Killing spinor equations, so BPS solutions found in one can be read in the other.
  • The reduced action reproduces the half-maximal gauged supergravity action, including the fermionic terms that had previously been written only for the bosonic sector.
  • The extra dual coordinates can be treated as physical, with dependence restricted to Scherk-Schwarz type, without spoiling local supersymmetry.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the Killing spinor equations really coincide, then the standard G-structure classification machinery used for ordinary supergravity could be applied directly to Scherk-Schwarz backgrounds of double field theory, which would give a systematic way to enumerate supersymmetric non-geometric backgrounds.
  • The correction term that reconciles the reduced and gauged actions, $tfrac12partial_M (U^{-1})^N{}_{hat Q}partial^M U^{hat Q}{}_P H^{NP}$, is bosonic only; the fermionic sector needs no such correction, which suggests the twist matrix enters supersymmetry purely through the projected spin connection.
  • Because the cancellation in (4.10) is asserted rather than displayed, an explicit term-by-term check with a simple twist matrix (for example a toroidal twist with constant $f_{ABC}$) would be a natural first test of the equivalence claim.
  • The construction is half-maximal; whether the same projection-based argument extends to the maximal or type II supersymmetric double field theory is left open by the paper and would be a natural next step.
Original abstract

Previous constructions of supersymmetry for double field theory have relied on the so called strong constraint. In this paper, the strong constraint is relaxed and the theory is shown to possess supersymmetry once the generalised Scherk-Schwarz reduction is imposed. The equivalence between the generalised Scherk-Schwarz reduced theory and the gauged double field theory is then examined in detail for the supersymmetric theory. As a byproduct we write the generalised Killing spinor equations for the supersymmetric double field theory.

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.

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,596 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.09 · states limitation 0.43 · human participants 0.01 · controlled comparison 0.06 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.93 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

Previous constructions of supersymmetry for double field theory have relied on the so called strong constraint. In this paper, the strong constraint is relaxed and the theory is shown to possess supersymmetry once the generalised Scherk-Schwarz reduction is imposed. The equivalence between the generalised Scherk-Schwarz reduced theory and the gauged double field theory is then examined in detail for the supersymmetric theory. As a byproduct we write the generalised Killing spinor equations for the supersymmetric double field theory.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Previous constructions of supersymmetry for double field theory have relied on the so called strong constraint. background 0.99 0.03 0.03 asserted 1.00
s1 In this paper, the strong constraint is relaxed and the theory is shown to possess supersymmetry once the generalised Scherk-Schwarz reduction is imposed. contribution 0.67 0.96 0.82 asserted 1.00
s2 The equivalence between the generalised Scherk-Schwarz reduced theory and the gauged double field theory is then examined in detail for the supersymmetric theory. contribution 0.98 0.90 0.14 asserted 0.88
s3 As a byproduct we write the generalised Killing spinor equations for the supersymmetric double field theory. result 0.66 0.95 0.06 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

What was examined, and what was not

sources read
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not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
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  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

References
How later papers used it

47 later papers cite it

Evidence: some. 37 of the citing papers share no author with it, and 5 of those carry a confident label from Pith's citation classifier.

Pith read 9 of the 85 citing sentences, choosing only those whose citation markers point at this paper alone, and wrote the paraphrases from them. The summary, the counts, the evidence level, the links and the quotes come from code; the summary counts the papers listed below. A later paper is listed under a label when Pith's citation classifier gives one of its sentences that label at probability 0.8 or more (0.95 for support), Pith's reading finds that the citing paper itself did it, and a second check confirms the paraphrase against the sentence. This section lists uses only. It does not list criticism or disagreement, so their absence here says nothing about how the paper has been received. Papers that share an author with this one are listed apart, under "By the same authors". A quote is the citing authors' own sentence, shown when their paper's licence is CC BY, CC BY-SA or CC0. JSON

Uses its method or tool 2 of 3 papers with this label · 2 by the same authors

By the same authors

How the literature uses it

47 arXiv papers cite this in 85 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 53 sentences without a confident label

Builds on it 1 paper
  • Finally let us mention that even if we have restricted our analysis to the bosonic sector of the heterotic string, the inclusion of fermions could also be addressed by invoking supersymmetry, generalizing the discussion in [ref] (see also [ref] ) where “will-be massless fermions at a fixed point”, specifically for modes in $Ǧ_n_c$, were considered.

    Symmetry enhancement interpolation, non-commutativity and Double Field Theory · Summary and Outlook · 0.82

Uses its method or tool 3 papers
  • In the present paper, utilizing the double-vielbein formalism for the supersymmetric gauged DFT [ref] , we investigate the supersymmetric structure of heterotic DFT up to quadratic order in $α'$, and we examine the validity of gauged DFT description in higher order corrections.

    Quadratic $\alpha'$-Corrections to Heterotic Double Field Theory · Introduction · 0.92

  • In order to halve them, as in [ref] , we may impose the following “gauged" section condition: (∂_A-i_A)(∂^A-i^A)=0 ,

    Standard Model as a Double Field Theory · Standard Model Double Field Theory (SM-DFT) · 0.91

  • Here, we follow the so called semi-covariant formalism [ref] which is well-suited for supersymmetry [See appendix [ref] for the concise review of double-vielbein formalism for gauged DFTs.]

    Effective Action for Non-Geometric Fluxes from Duality Covariant Actions · Nongeometric fluxes and action · 0.98

Compares with it 3 papers
Cites it as background 17 papers

What it cites · 35 sentences without a confident label

Builds on 2 papers
  • And so, we follow exactly the construction given in [ref] for non gauged DFT but now in this paper we will introduce a semi-covariant derivative for a twisted generalised Lie derivative ([ref]) which will be appropriate for a gauged theory.

    Differential geometry with a projection: Application to double field theory · Connection · 0.96

  • And so, we follow exactly the construction given in [ref] for non gauged DFT but now in this paper we will introduce a semi-covariant derivative for a twisted generalised Lie derivative ([ref]) which will be appropriate for a gauged theory.

    Stringy differential geometry, beyond Riemann · Connection · 0.96

Compares with 1 paper
  • This is the difference between reduced parent DFT connection $Γ̂_PMN$ in ([ref]) and gauged DFT connection $Γ_PMN$ in ([ref]) and it shows the origin in terms of the reduced connection of the additional term in the action that appeared in [ref] .

    Gauged Double Field Theory · Generalized Scherk-Schwarz reduced DFT as a gauged DFT · 0.95

Cites as background 55 papers

Discussion

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