Abstract

We complete the construction of a gauge-invariant action for NS-NS superstring field theory in the large Hilbert space begun in arXiv:1305.3893 by giving a closed-form expression for the action and nonlinear gauge transformations. The action has the WZW-like form and vertices are given by a pure-gauge solution of heterotic string field theory in the small Hilbert space.

Highlights

  • The cancellation of singularities can occur in the small Hilbert space

  • We find that using the elegant technique of [31], one can construct the WZW-like action for NS-NS superstring field theory in the large Hilbert space

  • A pure-gauge solution of small-space theory is the key concept of WZW-like formulation of NS superstring field theory in the large Hilbert space, which determines the vertices of theory, and we expect that it goes in the case of the NS-NS sector

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Summary

Nonlinear gauge invariance

We derive the equation of motion and the closed form expression of nonlinear gauge transformations. For example, GL(t = 0) = 0, GL(t = 1) = GL, Ψδ(t = 0) = 0, and Ψδ(t = 1) = Ψδ hold For this purpose, we prove that the variation δS does not includes t and is given by δS = Ψδ, η GL. The equation of motion is, given by (4.24) and it is independent of t-parametrization of fields. Since η GL is a QGL-, η-, and η-exact state, we find that the action is invariant under the following nonlinear Q- and η-gauge transformations and linear η-gauge transformation. An explicit expression for Q-gauge transformation δΛΨ and η-gauge transformation δΩΨ are given by δΛΨ. The action has three generators of gauge transformations, since one of these gauge invariances reduces to trivial, the resulting theory is Wess-Zumino-Wittenlikely formulated with two nonlinear gauge invariances

Cubic vertex
Quartic vertex
Gauge-invariant insertions of picture-changing operators
Coalgebraic description of vertices
Gauge-invariant insertions
NS string products
WZW-like expression
Pure-gauge GL and ‘large’ associated field ΨX
Wess-Zumino-Witten-like action
Conclusion
A Heterotic theory in the small Hilbert space
B Some identities
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