The Dyson equation and Green's function formalism map the problem of N electrons in the BornαOppenheimer nuclear field into a one-electron Schrodinger Γ«quation problem in quantum chemistry. The mass operator contains the information about electron correlation, and the ground-state energy, electron a
Vacuum polarization as spontaneous symmetry breaking
β Scribed by V. M. Nikolaenko
- Publisher
- John Wiley and Sons
- Year
- 1986
- Tongue
- English
- Weight
- 174 KB
- Volume
- 307
- Category
- Article
- ISSN
- 0004-6337
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β¦ Synopsis
On gaugingfrom a mechanical point of view ~'ontiiiuunr rireclr:iiiics 01 tlislocationh appears to I)c mi a1q)rol)riatc 1lrc.ory lor uiakiiig I 1 ~~1 1 1 s ~~i i r ~~i 1 1 1 IIC tiiwiiing ~l gCi~ifie lleltl procedures in it.
I he strcss functioti approach lo tlic thcory I)roduccs ;I freedom of pliasc traiislorniatioiis giviiig tlir coiiservatiuir of cliargc, rci)J-cxnted licrc by thc dislocation. f-lowcvcr, by minimal coupling neither this charge nor its iiclcl are cnlorcecl. only t1ic.y arc conipatiblc witli llrr theory. This means, the dislocation beconies the coupling constant for mechanical long-rangc interaction. Since this coupling appears to be a universal one for continuurn mechanics it can be givfn a pure geometrical meaniug. In this way the minimal coupling can be explained in terms of geometry by covariant derivatives. In &her 'cases this will not be possible -(elastic diel6ctrics 'for instance).' The coupling constant only translates tlic influcncc o f a spcci;il internal syniniclry 011 space-time by gauge-invariaiit derivatives .~iiiiiiiiiizing tlic influencr of a ncw [icltl on a givcn equation.
π SIMILAR VOLUMES
We construct a Lagrangian density which is manifestly invariant under the orthosymplectic gauge group OSP(l; 4) and under general coordinate transformations. This is done by the use of two multiplets, the symmetric and antisymmetric representations of OSP(l; 4). We present the general features of OS
A b s t r a c t . While for quantum field theoretical calculations it is sufficient to know the Lagrangian, we give here the field equations of the unified gauge-theory of weak and electromagnetic interactions after spontaneous symmetry breaking. With this approach, inhomogeneous Lorentz conditions