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　　String theory is one of the most exciting and challenging areas of modern theoretical physics. It was developed in the late 1960s for the purpose of de-scribing the strong nuclear force. Problems were encountered that prevented this program from attaining complete success. In particular, it was realized that the dpectrum of a fundamental string contains an undesired massless spin-two particle. Quantum chromodynamics eventually proved to be the correct theory for describing the strong force and the properties of hadr***,New doors opened for string theory when in 1974 it was proposed to identify the massless spin-two particle in the string's spectrum with the graviton, the quantum of gravitation. String theory became then the most promising can-didate for a quantum theory of gravity unified with the other forces and has developed into one of the most fascinating the6ries of high-energy physics.

preface

1 introduction

　1.1 historical origins

　1.2 general features

　1.3 basic string theory

　1.4 modern developments in superstring theory

2 the bosonic string

　2.1 p-brane acti***

　2.2 the string action

　2.3 string sigma-model action: the classical theory

　2.4 canonical quantization

　2.5 light-cone gauge quantization

3 conformal field theory and string in***cti***

　3.1 conformal field theory

　3.2 brst quantization

　3.3 background fields

　3.4 vertex operators

　3.5 the structure of string perturbation theory

　3.6 the linear-dilaton vacuum and noncritical strings

　3.7 witten's open-string field theory

4 strings with world-sheet supersymmetry

　4.1 ramond-neveu-schwarz strings

　4.2 global world-sheet supersymmetry

　4.3 c***traint equati*** mad conformal invaxiance

　4.4 boundary conditi*** and mode expansi***

　4.5 canonical quantization of the rns string

　4.6 light-cone gauge quantization of the rns string

　4.7 scft and brst

5 strings with space-time supersymmetry

　5.1 the do-brane action

　5.2 the supersymmetric string action

　5.3 quantization of the gs action

　5.4 gauge anomalies and their cancellation

6 t-duality and d-branes

　6.1 the bosonic string and dp-branes

　6.2 d-branes in type ii superstring theories

　6.3 type i superstring theory

　*** t-duality in the presence of background fields

　6.5 world-volume acti*** for d-branes

7 the het*** string

　7.1 nonabelian gauge symmetry in string theory

　7.2 fermionic c***truction of the het*** string

　7.3 toroidal compactification

　7.4 bosonic c***truction of the het*** string

8 m-theory and string duality

　8.1 low-energy effective acti***

　8.2 s-duality

　8.3 m-theory

　8.4 m-theory dualities

9 string geometry

　9.1 orbifolds

　9.2 calabi-yau manifolds: mathematical properties

　9.3 examples of calabi-yau manifolds

　9.4 calabi-yau compactificati*** of the het*** string

　9.5 deformati*** of calabi-yau manifolds

　9.6 special geometry

　9.7 type iia and type iib on calabi-yau three-folds

　9.8 nonperturbative effects in calabi-yau compactificati***

　9.9 mirror symmetry

　9.10 het*** string theory on calabi-yau three-folds

　9.11 k3 compactificati*** and more string dualities

　9.12 manifolds with g2 and spin(7) holonomy

10 flux compactificati***

　10.1 flux compactificati*** and calabi-yau four-folds

　10.2 flux compactificati*** of the type iib theory

　10.3 moduli stabilization

　10.4 fluxes, torsion and het*** strings

　10.5 the strongly coupled het*** string

　10.6 the landscape

　10.7 fluxes and cosmology

11 black ***s in string theory

　11.1 black ***s in general relativity

　11.2 black-*** thermodynamics

　11.3 black ***s in string theory

　11.4 statistical derivation of the entropy

　11.5 the attractor mechanism

　11.6 small bps black ***s in four dimensi***

12 gauge theory/string theory dualities

　12.1 black-brane soluti*** in string theory and m-theory

　12.2 matrix theory

　12.3 the ads/cft correspondence

　12.4 gauge/string duality for the conifold and generalizati***

　12.5 plane-wave space-times and their duals

　12.6 geometric transiti***

bibliographic discussion

bibliography

index

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书籍介绍

《弦论和M理论导论(英文版)》内容简介：String theory is one of the most exciting and challenging areas of moderntheoretical physics. It was developed in the late 1960s for the purpose of de- scribing the strong nuclear force. Problems were encountered that prevented this program from attaining complete success. In particular, it was realized that the spectrum of a fundamental string contains an undesired massless spimtwo particle. Quantum chromodynamics eventually proved to be the correct theory for describing the strong force and the properties of hadr***. New doors opened for string theory when in 1974 it was proposed to identify the massless spin-two particle in the string's spectrum with the graviton, the quantum of gravitation. String theory became then the most promising can didate for a quantum theory of gravity unified with the other forces and has developed into one of the most fascinating theories of high-energy physics.