1994
DOI: 10.1063/1.530703
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Vertex operators for physical states of bosonic string

Abstract: The commutator of the Virasoro operator Lm and general vertex operator V for the mass level L is explicitly calculated. By demanding that a physical vertex operator must be of conformal dimension J=1, a set of algebraic equations for determining the vertex operators corresponding to all physical states of bosonic strings is obtained. Explicit expressions for the first three mass levels are given.

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Cited by 4 publications
(10 citation statements)
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“…This will in turn confirm that the normalization of the functional representation of the coherent state (139), namely (144), is consistent with that obtained by operator methods, namely (140). Note furthermore, that the statement (161) is equivalent to the conformal field theory statement (28) that was derived by the ''one string in volume V dÀ1 '' requirement that leads to correctly normalized S-matrix elements.…”
Section: Consistency Checksupporting
confidence: 72%
See 1 more Smart Citation
“…This will in turn confirm that the normalization of the functional representation of the coherent state (139), namely (144), is consistent with that obtained by operator methods, namely (140). Note furthermore, that the statement (161) is equivalent to the conformal field theory statement (28) that was derived by the ''one string in volume V dÀ1 '' requirement that leads to correctly normalized S-matrix elements.…”
Section: Consistency Checksupporting
confidence: 72%
“…Various prescriptions have been given for the construction of covariant vertex operators, e.g. the construction due to Del Giudice, Di Vecchia and Fubini (DDF) [126][127][128][129] but see also [130], the path integral construction based on symmetry [131][132][133] and factorization [134][135][136] and operator constructions [137,138] among others. A powerful method which applies in general backgrounds is given in [139], (although explicit results for high mass states are seemingly rather difficult to obtain in more general backgrounds, see also [140,141]).…”
Section: H Vertex Operator Constructionsmentioning
confidence: 99%
“…For the low level states, the constraints are simple to solve, but they become increasingly cumbersome at higher levels, see e.g. [37][38][39][40]. Fortunately, there is a more systematic and physical approach: the DDF construction [41].…”
Section: Scattering Of Highly Excited Stringsmentioning
confidence: 99%
“…For the low level states, the constraints are simple to solve, but they become increasingly cumbersome at higher levels, see e.g. [35][36][37][38]. Fortunately, there is a more systematic and physical approach: the DDF construction [39].…”
Section: Scattering Of Highly Excited Stringsmentioning
confidence: 99%
“…37) and S n 1 ,n 2 (a function of q • ∂ m X) given in(3.43).Physically, the vertex operators are formed by starting with a tachyon of momentum p and scattering photons off of it (i.e. repeatedly taking the OPE with photon vertex operators) where the action of λ • A −m corresponds to a photon with polarization λ and momentum −mq where q • p = 1.…”
mentioning
confidence: 99%