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...
Збережено в:
Дата: | 2009 |
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Автор: | |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
2009
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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. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | 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. |
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