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Titlebook: General Principles of Quantum Field Theory; N. N. Bogolubov,A. A. Logunov,I. T. Todorov Book 1990 Kluwer Academic Publishers 1990 Cross se

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书目名称General Principles of Quantum Field Theory
编辑N. N. Bogolubov,A. A. Logunov,I. T. Todorov
视频video
丛书名称Mathematical Physics and Applied Mathematics
图书封面Titlebook: General Principles of Quantum Field Theory;  N. N. Bogolubov,A. A. Logunov,I. T. Todorov Book 1990 Kluwer Academic Publishers 1990 Cross se
描述The majority of the "memorable" results of relativistic quantum theory were obtained within the framework of the local quantum field approach. The explanation of the basic principles of the local theory and its mathematical structure has left its mark on all modern activity in this area. Originally, the axiomatic approach arose from attempts to give a mathematical meaning to the quantum field theory of strong interactions (of Yukawa type). The fields in such a theory are realized by operators in Hilbert space with a positive Poincare-invariant scalar product. This "classical" part of the axiomatic approach attained its modern form as far back as the sixties. * It has retained its importance even to this day, in spite of the fact that nowadays the main prospects for the description of the electro-weak and strong interactions are in connection with the theory of gauge fields. In fact, from the point of view of the quark model, the theory of strong interactions of Wightman type was obtained by restricting attention to just the "physical" local operators (such as hadronic fields consisting of ‘‘fundamental‘‘ quark fields) acting in a Hilbert space of physical states. In principle, ther
出版日期Book 1990
关键词Cross section; Dirac equation; Observable; Quark; Second quantization; classification; statistics
版次1
doihttps://doi.org/10.1007/978-94-009-0491-0
isbn_softcover978-94-010-6707-2
isbn_ebook978-94-009-0491-0
copyrightKluwer Academic Publishers 1990
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Monotreme and Marsupial Placentation,ress tensor field .(.) satisfying Maxwell’s equations. This state can also be defined by a vector potential .(.); however, such a characterization has a certain redundancy since two configurations, say, .(.) and .′.(.)of the vector potential define the same physical state (that is, they are equivalent) if their stress tensor fields are the same:
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