An introduction to the theory of groups of finite order by Harold Hilton
By Harold Hilton
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The contents of this ebook were used in classes given through the writer. the 1st used to be a one-semester path for seniors on the college of British Columbia; it used to be transparent that sturdy undergraduates have been completely in a position to dealing with user-friendly team concept and its program to basic quantum chemical difficulties.
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P → ν + p, νµ + e → νµ + e, νe + e → νe + e. 11) These processes have been observed  and they conﬁrm eq. 9) as the correct structure for the weak Hamiltonian up to a piece, which we denote by Hwk : 4GF Hwk = − √ k¯ ν γ µ (1 + γ5 )νJµem . 12) If we temporarily ignore eq. 12), we ﬁnd that the weak interaction Hamiltonian has all the right properties to incorporate an underlying local weak SU(2) symmetry. Under this weak SU(2) symmetry, the left-handed fermions must transform as doublets as follows: νeL uL d cos θ e− L C + sL sin θC L νµL .
14, 1047 (1965).  C. N. Yang and R. L. Mills, Phys. Rev. 96, 191 (1954).  R. D. Thesis, Cambridge University, 1955.  O. W. Greenberg, Phys. Rev. Lett. 13, 598 (1964); M. Y. Han and Y. Nambu, Phys. Revs. 139, B1006 (1965). For a review and references on the subject, see O. W. Greenberg and C. A. Nelson, Phys. Rep. 32, 69 (1977); W. Marciano and H. Pagels, Phys. Rep. 36C, 137 (1978).  J. D. Bjorken, Phys. Rev. 179, 1547 (1969).  R. , 1972.  J. D. Bjorken and E. A. Paschos, Phys.
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