Epstein Secrets

yet to be found. Another issue which should be addressed is that of the representations content of the SU(212) symmetry uncovered for the superfiag Landau model [9], within the study of quantum mechanics on super manifolds. Preliminary results indicate these are new types of short representations previ

litated obtaining analytic results as well as a numerical study of this special model. The supersymmetric system in question is given by a cube root Lagrangian, and a corresponding double-valued Hamiltonian. L=C(v-1)13—V(x) e=:- Legendre Ht d2 = 1L) + V (x) , V (x) = 22 — (1) 2Vp Q111 in p space

lid varies with 41. We find that 14„r also changes at a level comparable to its sensitivity to Mg or Ali as the gauge pa- rameter deviates from the Landau gauge (egc = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in lid is far

ng for the Higgs field, G = -4 $t4,R, where 4> is the Higgs dou- blet and R the Ricci scalar. One can remove the non-minimal coupling term from the Lagrangian by performing a confor- mal transformation, 9,,,(x) = r1-2(x)§0,(x) where 122 = 1 + 2e4)t./All, (2) is the conformal factor and Alp is the reduced

ia varies with $4e. We find that V;,,( also changes at a level comparable to its sensitivity to Ahr or Me as the gauge pa- rameter deviates from the Landau gauge (‘ = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in Vim is far t

g for the Higgs field. C = ciblibR. where (ff is the Higgs dou- blet and R the Ricci scalar. One can remove the non-minimal coupling term from the Lagrangian by performing a confor- mal transformation, go,„(x) = 51-2(x)li,„(s) where D2 = 1 + 2e(}141/4/1, (2) is the conformal factor and My is the reduced