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Gauge-invariant operators of open bosonic string field theory in the low-energy limit

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arxiv 2006.16710 v1 pith:WGJGI6KC submitted 2020-06-30 hep-th

Gauge-invariant operators of open bosonic string field theory in the low-energy limit

classification hep-th
keywords operatorsgauge-invariantlimitlow-energyopenstringactionfield
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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In the AdS/CFT correspondence we consider correlation functions of gauge-invariant operators on the gauge theory side, which we obtain in the low-energy limit of the open string sector. To investigate this low-energy limit we consider the action of open bosonic string field theory including source terms for gauge-invariant operators and classically integrate out massive fields to obtain the effective action for massless fields. While the gauge-invariant operators depend linearly on the open string field and do not resemble the corresponding operators such as the energy-momentum tensor in the low-energy limit, we find that nonlinear dependence is generated in the process of integrating out massive fields. We also find that the gauge transformation is modified in such a way that the effective action and the modified gauge transformation can be written in terms of the same set of multi-string products which satisfy weak $A_\infty$ relations, and we present explicit expressions for the multi-string products.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Higher Connection in Open String Field Theory

    hep-th 2026-02 unverdicted novelty 7.0

    A 2-form connection is defined in the space of open string field theory solutions, producing invariant higher holonomies and 3-form curvature potentially corresponding to the B-field.

  2. Homotopy transfer for massive Kaluza-Klein modes

    hep-th 2025-12 unverdicted novelty 7.0

    An algorithm based on homotopy transfer in L∞ algebras produces gauge-invariant fields for massive Kaluza-Klein modes that remain covariant under unbroken zero-mode gauge transformations.