1996
DOI: 10.1142/s0217732396001405
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FINITE Q-OSCILLATOR REPRESENTATION OF 2-D STRING THEORY

Abstract: We present a simple physical representation for states of two-dimensional string theory. In order to incorporate a fundamental cutoff of the order 1/g st we use a picture consisting of q-oscillators at the first quantized level. In this framework we also find a representation for the (singular) negatively dressed states representing nontrivial string backgrounds.Of some importance is the difference between the states of positive Liouville dressing Ψ (+) versus those of negative dressing Ψ (−) . The former are … Show more

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Cited by 16 publications
(19 citation statements)
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“…Using the match of KK states with generating chiral primaries [7], the cutoff on such chiral primaries in the CFT was analyzed and shown to be in agreement with the above SU q (2) × SU q (1, 1) spacetime. Another way to arrive at the same value of q was dynamical as in similar work in earlier matrix models [8]. An SL q (2) subalgebra was identified in the algebra generated by the chiral primaries and their conjugates.…”
Section: Introductionmentioning
confidence: 94%
“…Using the match of KK states with generating chiral primaries [7], the cutoff on such chiral primaries in the CFT was analyzed and shown to be in agreement with the above SU q (2) × SU q (1, 1) spacetime. Another way to arrive at the same value of q was dynamical as in similar work in earlier matrix models [8]. An SL q (2) subalgebra was identified in the algebra generated by the chiral primaries and their conjugates.…”
Section: Introductionmentioning
confidence: 94%
“…The connection between Symmetric and Unitary groups was crucial in the development of the String theory of two-dimensional Yang Mills Theory [17,18,19,20,21,22,23,24] and in certain aspects of Low-dimensional Matrix Models [25,26]. Some key useful results are collected here.…”
mentioning
confidence: 99%
“…Then we can restrict the algebra by a † a = φ(N)θ(N), where θ(N) is 0 or 1, depending on whether the given N -particle (excitation) state is forbidden or allowed. The simplest case [22] is θ(n) = 1, n ≤ p and θ(n) = 0, n > p.…”
Section: Restricted Algebras and Projected Fock Spacesmentioning
confidence: 99%
“…Generally, the Gentile-type statistics can be defined by As example, we consider restricted Bose oscillator 5) with Fock space spanned by |0 >, a † |0 >, ...(a † ) m |0 >. This oscillator coincides with the truncated Bose oscillator with cutoff [22] aa † = (1 + a † a) − (N + 1) δ N,m (4.6) or aa † = Θ(m − N + 1). The counting rule is…”
Section: Gentile -Type Statistics : Restrictions On Each Single Oscilmentioning
confidence: 99%