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.0708. [9] A. De Simone. M. P. Hertzberg. and F. Wilczek. Phys.Lett. B678. 1 (2009). arXiv:0812.4946. [1
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 (2014). arXiv:1309.5343. [52] B. M. Kastening. Phys.Lett. 11283, 287 (1992). [53] M. Bando. T Kugo, N. Maekawa. and H. Naka
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
Some examples of brandied Hamiltonians were explored both classically and in the context of quan- tum mechanics, as recently advocated by Shapere and Wilczek. These are in fact cases of switch- back potentials, albeit in momentum space, as previously analyzed by us for quasi-Hamiltonian chaotic dynamical
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
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 (2014), arXiv:1309.5343. 52] B. M. Kastening. Phys.Lett. B283. 287 (1992). 53] M. Bando. T. Kugo, N. Maekawa. and H. Nakano
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
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Green
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Australian National University
ORGANIZATIONHiggs
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