Topologically distinct Feynman diagrams for mass operator in electron-phonon interaction

The new method for designing topologically distinct Feynman diagrams for electron's mass operator in electronphonon interaction is developed using the permutation group theory. The carried out classification of DPs allows to choose the classes, corresponding to disconnected diagrams, to singl...

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Збережено в:
Бібліографічні деталі
Дата:2009
Автор: Tovstyuk, C.C.
Формат: Стаття
Мова:English
Опубліковано: Інститут фізики конденсованих систем НАН України 2009
Назва видання:Condensed Matter Physics
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/119990
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Topologically distinct Feynman diagrams for mass operator in electron-phonon interaction / C.C. Tovstyuk // Condensed Matter Physics. — 2009. — Т. 12, № 2. — С. 225-238. — Бібліогр.: 14 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Резюме:The new method for designing topologically distinct Feynman diagrams for electron's mass operator in electronphonon interaction is developed using the permutation group theory. The carried out classification of DPs allows to choose the classes, corresponding to disconnected diagrams, to singly connected diagrams, direct ( tadpole ) diagrams, to diagrams corresponding to phonon Green functions. After this classification the set of considered double permutations is reduced to one class since only these are relevant to mass operator. We derive analytical expressions which allow to identify the DP, and to choose the phonon components, which are not accepted in every type. To avoid repetition of asymmetric diagrams, which correspond to the same analytical expression, we introduce the procedure of inversion in phonon component, and identify symmetric as well as a pair of asymmetric phonon components. For every type of DP (denoted by its digital encoding), taking into account its symmetry, we perform a set of transformations on this DP, list all DPs of the type and all the corresponding Feynman diagrams of mass operator automatically. It is clear that no more expressions (diagrams) for the relevant order of perturbation theory for mass operator can be designed.