Epstein Secrets

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

0) 321]. [141] D. V. Volkov, "Quartions in relativistic field theory", .JETP Lett. 49 (1989) 541 [Pisma Zh. Eksp. Thor. Fiz. 49 (1989) 473]. [142] E. J. Weinberg, "Multivortex Solutions Of The Ginzburg-Landau Equations," Phys. Rev. D 19 (1979) 3008. [143] F. Wilczek, "Fractional statistics and anyon supercon

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

arXiv:1112.2659. 48] K. Kamada. T. Kobayashi. M. Yamaguchi, and J. Yokoyama, Phys.Rev. D83. 083515 (2011). arXiv:1012.4238. 49] S. R. Coleman and E. J. Weinberg, Phys.Rev. D7, 1888 (1973). 50] D. I. Kaiser. Phys.Rev. D81, 084044 (2010), arXiv:1003.1159. 51] L. M. Krauss and F Wilczek, Phys.Rev. D89. 047501

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

arXiv:1112.2659. 1481 K. Kamada. T. Kobayashi. M. Yamaguchi. and J. Yokoyama, Phys.Rev. D83.083515 (2011), arXiv:1012.4238. 149] S. R. Coleman and E. J. Weinberg, Phys.Rev. D7. 1888 (1973). [50] D. I. Kaiser. Phys.Rev. D81.084044 (2010), arXiv:1003.1159. 151] L. M. Krauss and E Wilczek. Phys.Rev. D89. 047501