2004
DOI: 10.1016/j.nuclphysb.2003.10.037
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Physical states at the tachyonic vacuum of open string field theory

Abstract: We illustrate a method for computing the number of physical states of open string theory at the stable tachyonic vacuum in level truncation approximation. The method is based on the analysis of the gauge-fixed open string field theory quadratic action that includes Fadeev-Popov ghost string fields. Computations up to level 9 in the scalar sector are consistent with Sen's conjecture about the absence of physical open string states at the tachyonic vacuum. We also derive a long exact cohomology sequence that rel… Show more

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Cited by 24 publications
(60 citation statements)
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“…These are the null vectors responsible for the poles of the string field propagators. The approximately degenerate poles that we found numerically correspond in the exact theory to a null space 3 In [1] it was established that a certain number of different assignments for the relative cohomologies, all of which implied (1.5), were consistent with the long exact sequence. The analysis could not provide a unique possibility for the explicit representatives of the absolute cohomologies.…”
Section: Introduction Summary and Discussionmentioning
confidence: 64%
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“…These are the null vectors responsible for the poles of the string field propagators. The approximately degenerate poles that we found numerically correspond in the exact theory to a null space 3 In [1] it was established that a certain number of different assignments for the relative cohomologies, all of which implied (1.5), were consistent with the long exact sequence. The analysis could not provide a unique possibility for the explicit representatives of the absolute cohomologies.…”
Section: Introduction Summary and Discussionmentioning
confidence: 64%
“…In [1] we explained what Sen's third conjecture implies for the gaugefixed quadratic OSFT action expanded around the stable vacuum: each pole of the open string field propagator should cancel with appropriate poles of the (second quantized) ghost string fields. To state it more precisely, let us denote by L (n) 0 (p) (where n = 0, 1, .…”
Section: Introduction Summary and Discussionmentioning
confidence: 95%
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