2000
DOI: 10.1103/physrevlett.85.3343
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Matrix Theory Interpretation of Discrete Light Cone Quantization String Worldsheets

Abstract: We study the null compactification of type-IIA-string perturbation theory at finite temperature. We prove a theorem about Riemann surfaces establishing that the moduli spaces of infinite-momentum-frame superstring worldsheets are identical to those of branched-cover instantons in the matrix-string model conjectured to describe M-theory. This means that the identification of string degrees of freedom in the matrix model proposed by Dijkgraaf, Verlinde and Verlinde is correct and that its natural generalization … Show more

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Cited by 25 publications
(46 citation statements)
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“…(5.18) and (5.23) there), has been subsequently and independently derived in [5] by studying the null compactification of type-IIA-string perturbation theory at finite temperature. In [5] an equivalent proof of Theorem 3 is also provided.…”
Section: Theorem 2 If the Holomorphic One-differentials ω Nm And ω mentioning
confidence: 99%
“…(5.18) and (5.23) there), has been subsequently and independently derived in [5] by studying the null compactification of type-IIA-string perturbation theory at finite temperature. In [5] an equivalent proof of Theorem 3 is also provided.…”
Section: Theorem 2 If the Holomorphic One-differentials ω Nm And ω mentioning
confidence: 99%
“…It is interesting to ask whether one can characterize this subset in a convenient way. In this Section we will review a theorem about the classification which was proved in [2]. A hint about this classification can be found by counting the number of moduli of the Riemann surface that eqn.…”
Section: Type II Superstring At Genusmentioning
confidence: 99%
“…This result was first obtained in ref. [2]. Since the first homology group of the 2-sphere is trivial, the first order in perturbation theory which is affected is at genus 1.…”
Section: Dlcq Of the String: Path Integralmentioning
confidence: 99%
“…This equivalence may be given a geometric interpretation by introducing a finite temperature [31,33]. This is done by further compactifying Euclidean time so that two target space directions are compactified on a torus T 2 τ of a particular modulus τ .…”
Section: Introductionmentioning
confidence: 99%
“…For the present discussion, the thermodynamic partition function is simply regarded as a generating function for the energy spectrum of free string theory and thermal instabilities such as the gravitational Jeans instability or the stringy Hagedorn transition will be ignored. On the Type IIA side, the one-loop free energy is given by a sum over unramified coverings of the torus T 2 τ of degree N [31,33]. On the superconformal field theory side, the partition function on T 2 τ is given by a sum over twisted sectors imposing S N -twisted boundary conditions on the string embedding fields.…”
Section: Introductionmentioning
confidence: 99%