Download PDF by Mazurov V. D.: 2-Signalizers of finite groups

By Mazurov V. D.

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Phys. B199 (1982) 36. 9] L. Maiani in Proc. Gif-sur-Yvette Summer School (Paris, 1980), p3. E. Witten, Nucl. Phys. B88 (1981) 513. M. Veltman, Acta. Phys. Polon. B12 (1981) 437. 10] P. Fayet, Phys. Lett. B64 (1976) 159; ibid. B69 (1977) 489; Recherche 19 (1988) 304; Ecole Normale Superieure Report No. LPTENS-94-90 (1994). E. L. Kane, loc. , Bibl. D. M. Lifshitz, # 1 , op. cit, Bibl. J. Sakurai, op. , Bibl. W. Heitler, op. , Bibl. F. Weisskopf, Phys. Rev. 56 (1939) 72. D. D. Drell, op. cit, Bibl.

Dk ' Tr ( _ i 4 i4(o) (2TT)4" V A "\/2/ y/2) rrif # $-m} 2 k + m) i\2 f d k f J (2TT^ (2^ 4 C? 4) is quadratically divergent and is moreover independent of the scalar mass ms- First of all, this divergence is very severe. 2. 4 x 1018 GeV, the highest scale known in physics. 15], by the requirement of perturbative unitarity in the amplitude W+W~ —>• W+W~, to be < O (1 TeV). 4) being independent of ms is an indication of the fact that ms is an unnatural parameter in the SM. Setting ms — 0 does not increase the symmetry of that theory.

13) assumes great significance when these considerations are extended to an uncountable infinity of harmonic oscillators as occur in field theory. 14b) 5^ = (iq - ojq)e . 16a) We use the notation [A, B] = AB- BA, [A, B]+ = AB + BA . One needs to anticommute the partial derivative with respect to i/> through the ip^ factor in the first term of Lp. 3 2. Preliminaries 24 Q = (iq - uq)tp = -y/^ua'b . 14a) Sq must be real which means that ijj^e has to be the hermitian conjugate of eip. 16) that the hermitian conjugate of eQ is — eQ here so that eQ + eQ is antihermitian.

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2-Signalizers of finite groups by Mazurov V. D.

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