2003
DOI: 10.1140/epjc/s2003-01336-8
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A note on effective N = 1 super-Yang-Mills theoriesversus lattice results

Abstract: We compare the glueball mass spectrum of an effective N = 1 pure super Yang-Mills theory formulated in terms of a three-form supermultiplet with the available lattice data. These confirm the presence of four scalars and two Majorana fermions but the detailed mass spectrum is difficult to reconcile with the effective supersymmetric theory. By imposing supersymmetry and using two of four bosonic masses we get a prediction for the remaining masses as well as the mixing angles. We find that the mass of the three-f… Show more

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Cited by 18 publications
(37 citation statements)
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“…The mass difference between states of opposite parity is bigger than the gluino mass used for the simulations [25]. This implies that it does not seem to be an effect of softly broken supersymmetry, as has been also stressed in [18].…”
Section: Spectrum Of Super Yang-mills Theory From Lattice Resultsmentioning
confidence: 88%
“…The mass difference between states of opposite parity is bigger than the gluino mass used for the simulations [25]. This implies that it does not seem to be an effect of softly broken supersymmetry, as has been also stressed in [18].…”
Section: Spectrum Of Super Yang-mills Theory From Lattice Resultsmentioning
confidence: 88%
“…The VY Lagrangian concisely summarizes the symmetries of the underlying theory in terms of a "minimal" number of degrees of freedom whose choice is not unambiguous. Generalizations of the VY Lagrangian containing more degrees of freedom were discussed in the literature [21,22]. These extensions were triggered, in part, by lattice simulations of SYM spectrum [23].…”
Section: Reviewing Sym Effective Lagrangianmentioning
confidence: 99%
“…However the program of including the purely gluonic operators ("glueballs") as dynamical degrees of freedom turns out to be non trivial [2,3,4,5]. In [2,4,5] the Veneziano-Yankielowicz low energy Lagrangian was extended so as to include all the desired low energy states, which are arranged into two Wess-Zumino supermultiplets. The authors of [3] pointed out on the other hand, that fulfillment of the program requires dynamical SUSY breaking and its consequent absence from the particle spectrum.…”
Section: Introductionmentioning
confidence: 99%