Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics
Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics
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In our eReader you can find the full English version of the book. Read Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics
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The function, G Q , approaches a constant equal to unity. Therefore the approximation used to derive the 2 M.S.S. not only holds but is actually better in the asymptotic p region 113 than it is in the mass shell region. By this criterion alone the M.S.S.
2 should be expected to work in the asymptotic p region.
However, in deriving the M.S.S. another approximation was made.
It was assumed A(p^) ■ A(p|) -m, (8-8) where m is the experimental mass. This approximation is completely 2 wrong in the la...rge p region since as |p 2 |+~, A(p^) + and A(p 2 ) - 0. (8-9) In deriving the M.S.S. as it appears in Table 6-1, the approxima- tion in Eq. (8-8) was used to provide a simplified expression of the D A , D A , D A and D A tensors (first defined in Eq. (6-7)). If the approx- y' yv yvp imation had not been employed the tensors, D , D , D and D , would have taken the form, D A = [A ]P A + A 2 p A ]/D 12 !2 C = [(p ly p 2v " P 2 yPlX + (Plv P 2p-P2vPlp )6 y + (p.
What to read after Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics?
You can find similar books in the "Read Also" column, or choose other free books by Cartier, Joan F. to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
The function, G Q , approaches a constant equal to unity. Therefore the approximation used to derive the 2 M.S.S. not only holds but is actually better in the asymptotic p region 113 than it is in the mass shell region. By this criterion alone the M.S.S.
2 should be expected to work in the asymptotic p region.
However, in deriving the M.S.S. another approximation was made.
It was assumed A(p^) ■ A(p|) -m, (8-8) where m is the experimental mass. This approximation is completely 2 wrong in the la...rge p region since as |p 2 |+~, A(p^) + and A(p 2 ) - 0. (8-9) In deriving the M.S.S. as it appears in Table 6-1, the approxima- tion in Eq. (8-8) was used to provide a simplified expression of the D A , D A , D A and D A tensors (first defined in Eq. (6-7)). If the approx- y' yv yvp imation had not been employed the tensors, D , D , D and D , would have taken the form, D A = [A ]P A + A 2 p A ]/D 12 !2 C = [(p ly p 2v " P 2 yPlX + (Plv P 2p-P2vPlp )6 y + (p.
What to read after Solution to the Schwinger-Dyson Equations of Quantum Electrodynamics?
You can find similar books in the "Read Also" column, or choose other free books by Cartier, Joan F. to read onlineMoreLess
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