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We consider the $N=(1,1)$ SYM theory that is obtained by dimensionallyreducing SYM theory in 2+1 dimensions to 1+1 dimensions and discuss softsupersymmetry breaking. We discuss the numerical simulation of this theoryusing SDLCQ when either the boson or the fermion has a large mass. We compareour result to the pure adjoint fermion theory and pure adjoint boson DLCQcalculations of Klebanov, Demeterfi, and Bhanot and of Kutasov. With a largeboson mass we find that it is necessary to add additional operators to thetheory to obtain sensible results. When a large fermion mass is added to thetheory we find that it is not necessary to add operators to obtain a sensibletheory. The theory of the adjoint boson is a theory that has stringy boundstates similar to the full SYM theory. We also discuss another theory ofadjoint bosons with a spectrum similar to that obtained by Klebanov, Demeterfi,and Bhanot.Comment: 12 pages, 4 figure

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

Numerical simulations of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mn>1</mml:mn><mml:mo>)</mml:mo><mml:mn /><mml:mi /><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:math>-dimensional super Yang-Mills theory with large supersymmetry breaking

Numerical simulations ofN=(1,1)1+1-dimensional super Yang-Mills theory with large supersymmetry breaking