1990
DOI: 10.1016/0550-3213(90)90032-9
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The decay of highly excited closed strings

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Cited by 41 publications
(62 citation statements)
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“…This formula nicely encompass all the particle width decays in the standard model (muons, Higgs, etc), as well as the decay width of topological and non topological solitons, cosmic defects and fundamental quantum strings [19]. A quantum closed string in an Nth excited state decays into lower excited states (including the dilaton, graviton and massless antisymmetric tensor fields) with a total width (to the dominant order (one string loop)) given by [20] …”
Section: Unified Quantum Decay Of Qft Elementary Particles Black mentioning
confidence: 99%
“…This formula nicely encompass all the particle width decays in the standard model (muons, Higgs, etc), as well as the decay width of topological and non topological solitons, cosmic defects and fundamental quantum strings [19]. A quantum closed string in an Nth excited state decays into lower excited states (including the dilaton, graviton and massless antisymmetric tensor fields) with a total width (to the dominant order (one string loop)) given by [20] …”
Section: Unified Quantum Decay Of Qft Elementary Particles Black mentioning
confidence: 99%
“…Traditionally, these are described in a mass eigenstate basis, and calculations almost exclusively [10][11][12][13][14][15][16][17] focus on leading Regge trajectory states which do not exhibit generic features (such as non-degenerate cusps [27]). Although physical vertex operators for arbitrary mass eigenstates are known [9], they are not a natural basis for highly excited strings as the resulting amplitudes generically become unwieldy.…”
mentioning
confidence: 99%
“…Decay rates may be extracted from the imaginary part of two-point amplitudes [10][11][12][13][14][15] [32,33,35]. When strings in the loops go onshell, they can appear in final states.…”
mentioning
confidence: 99%
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