Symmetry Laws and Strong Interactions

نویسندگان

  • L. Wolfenstein
  • D. G. Ravenhall
چکیده

where Re means "real part. " It is easy to see that P(x) is the time rate of change at which the electric field does work per unit volume on the sources. Hence S'= (1/Ssr) g;lb;*lb; is the energy density and the components S' (a=1, 2, 3) are the components of the Poynting vector. Since the field P is arbitrary, we can strip off the integrals in (9) and obtain the familiar diGerential form of the conservation of energy:

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تاریخ انتشار 2011