1999
DOI: 10.1063/1.1301663
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SDLCQ supersymmetric discrete light cone quantization

Abstract: In these lectures we discuss the application of discrete light cone quantization (DLCQ) to supersymmetric field theories. We will see that it is possible to formulate DLCQ so that supersymmetry is exactly preserved in the discrete approximation. We call this formulation of DLCQ, SDLCQ and it combines the power of DLCQ with all of the beauty of supersymmetry. In these lecture we will review the application of SDLCQ to several interesting supersymmetric theories. We will discuss two dimensional theories with (1,… Show more

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Cited by 37 publications
(48 citation statements)
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“…This property is interesting because reduced N = 1 SYM theories are very stringy theories. The low-mass states are dominated by Fock states with many constituents, and as the size of the superalgebraic representation is increased, states with lower masses and more constituents appear [1,2,9,11,12,13,14,15,16,17,18,19,20]. The connection between string theory and supersymmetric gauge theory leads one to expect this type of behavior.…”
Section: Introductionmentioning
confidence: 99%
“…This property is interesting because reduced N = 1 SYM theories are very stringy theories. The low-mass states are dominated by Fock states with many constituents, and as the size of the superalgebraic representation is increased, states with lower masses and more constituents appear [1,2,9,11,12,13,14,15,16,17,18,19,20]. The connection between string theory and supersymmetric gauge theory leads one to expect this type of behavior.…”
Section: Introductionmentioning
confidence: 99%
“…There is a host of results in SDLCQ in two and three dimensions on correlators [1], bound states [2], and other topics, including an overview article, Ref. [3].…”
Section: Introducing the Method: Sdlcqmentioning
confidence: 99%
“…Specifically, we calculate the compositions Thus, taking into account the several types of partons that can form C 5 3 , the total number of states we get for this case is 2 3 3 2 1 48. The total number of states-including the massless ones-as a function of K is thus…”
Section: A Limiting Casesmentioning
confidence: 99%
“…We have discussed the SDLCQ numerical method in a number of other places, and we will not present a detailed discussion of the method here; for a review, see [5]. For those familiar with DLCQ [14,15], it suffices to say that SDLCQ is similar; both impose periodic boundary conditions on a light-cone box x ÿ 2 ÿL; L and have discrete momenta and cutoffs in momentum space.…”
Section: Introductionmentioning
confidence: 99%
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