Abstract

We compute semi-classical corrections to the energy of rotating closed Nambu-Goto strings. We confirm the results obtained by means of the Polchinski-Strominger action. We also show that in this semi-classical approximation, the spectrum of physical excitations contains modes that are unphysical non-perturbatively, i.e., to which no physical excitations of the covariantly quantized Nambu-Goto string correspond.

Highlights

  • In the covariant quantization scheme, the Regge intercept a of the Nambu-Goto string is a free parameter, only constrained by a ≤ 1 for D ≤ 25 and a 1⁄4 1 for D 1⁄4 26, with D the dimension of the target Minkowski space [1,2]

  • We show that in this semiclassical approximation, the spectrum of physical excitations contains modes that are unphysical nonperturbatively, i.e., to which no physical excitations of the covariantly quantized Nambu-Goto string correspond

  • We show that for the closed string the spectrum of excitations in the semi-classical theory is too large, i.e., there are semi-classical excitations that do not correspond to physical excitations of the full nonperturbative covariantly quantized theory

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Summary

INTRODUCTION

In the covariant quantization scheme, the Regge intercept a of the Nambu-Goto string is a free parameter, only constrained by a ≤ 1 for D ≤ 25 and a 1⁄4 1 for D 1⁄4 26, with D the dimension of the target Minkowski space [1,2]. The equations of motion for φ only depend on the world sheet geometric data, i.e., the metric and the second fundamental form induced by the classical embedding X It seems natural, in line with the framework of [11], to use methods from quantum field theory on curved space-time [14,15] for the renormalization of the free world sheet Hamiltonian H0. An Appendix contains some intermediate results of our treatment of the elliptic case

PERTURBATIONS OF CLASSICAL ROTATING CIRCULAR STRINGS
THE WORLD SHEET HAMILTONIAN
Tr þ tA0 þ ðA0A0 t2 þ
GENERALIZATION TO THE ELLIPTIC CASE
THE GENERALIZATION TO ARBITRARY DIMENSIONS
THE SPECTRUM OF PHYSICAL EXCITATIONS
CONCLUSION
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