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Unformatted text preview: arXiv:hepth/9612114v1 11 Dec 1996 FERMILABPUB96/445T INTRODUCTION TO SUPERSYMMETRY JOSEPH D. LYKKEN Fermi National Accelerator Laboratory P.O. Box 500 Batavia, IL 60510 These lectures give a selfcontained introduction to supersymmetry from a modern perspective. Emphasis is placed on material essential to understanding duality. Topics include: central charges and BPSsaturated states, supersymmetric nonlin ear sigma models, N=2 YangMills theory, holomorphy and the N=2 YangMills β function, supersymmetry in 2, 6, 10, and 11 spacetime dimensions. 1 Introduction “Never mind, lads. Same time tomorrow. We must get a winner one day.” – Peter Cook, as the doomsday prophet in “The End of the World”. Supersymmetry, along with its monozygotic sibling superstring theory, has become the dominant framework for formulating physics beyond the standard model. This despite the fact that, as of this morning, there is no unambiguous experimental evidence for either idea. Theorists find supersymmetry appealing for reasons which are both phenomenological and technical. In these lectures I will focus exclusively on the technical appeal. There are many good recent re views of the phenomenology of supersymmetry. 1 Some good technical reviews are Wess and Bagger, 2 West, 3 and Sohnius. 4 The goal of these lectures is to provide the student with the technical back ground requisite for the recent applications of duality ideas to supersymmetric gauge theories and superstrings. More specifically, if you absorb the material in these lectures, you will understand Section 2 of Seiberg and Witten, 5 and you will have a vague notion of why there might be such a thing as Mtheory. Beyond that, you’re on your own. 2 Representations of Supersymmetry 2.1 The general 4dimensional supersymmetry algebra A symmetry of the Smatrix means that the symmetry transformations have the effect of merely reshuffling the asymptotic single and multiparticle states. The known symmetries of the Smatrix in particle physics are: 1 • Poincar´ e invariance, the semidirect product of translations and Lorentz rotations, with generators P m , M mn . • Socalled “internal” global symmetries, related to conserved quantum numbers such as electric charge and isospin. The symmetry generators are Lorentz scalars and generate a Lie algebra, [ B ℓ ,B k ] = iC j ℓk B j , (1) where the C j ℓk are structure constants. • Discrete symmetries: C, P, and T. In 1967, Coleman and Mandula 6 provided a rigorous argument which proves that, given certain assumptions, the above are the only possible sym metries of the Smatrix. The reader is encouraged to study this classic paper and think about the physical and technical assumptions which are made there....
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This note was uploaded on 05/17/2011 for the course PHYSICS 123 taught by Professor Hayes during the Spring '07 term at Harvard.
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