Titlebook: Renormalization Theory; Proceedings of the N G. Velo,A. S. Wightman Conference proceedings 1976 D. Reidel Publishing Company, Dordrecht, Ho

negation

书目名称Renormalization Theory影响因子(影响力)




书目名称Renormalization Theory影响因子(影响力)学科排名




书目名称Renormalization Theory网络公开度




书目名称Renormalization Theory网络公开度学科排名




书目名称Renormalization Theory被引频次




书目名称Renormalization Theory被引频次学科排名




书目名称Renormalization Theory年度引用




书目名称Renormalization Theory年度引用学科排名




书目名称Renormalization Theory读者反馈




书目名称Renormalization Theory读者反馈学科排名

无节奏

faddish

BALE

Quantum Sine-Gordon Equation and Quantum Solitons in Two Space-Time Dimensions,I study mainly the construction and the detailed properties of a new model of a self-interacting, relativistic scalar Bose field in two space- time dimensions: the quantum sine-Gordon equation (≡ s-G theory).

硬化

Non-Perturbative Renormalization in the Yukawa Model In Two Dimensions,tes for more information [VW]) the next model in line is Y2, the “first“ one to require some real renormalization. The next step after that,ø. which is even more singular, will be discussed by J. Feldman. The major complication in Y., and at the same time the reason why it can be handled, as we shall see later, is the appearance of fermions.

recede

Orientation,nd technical subject. As a result it is easy to lose sight of the main themes in the welter of details. In the hope of making the theory more accessible to the earnest student, I shall not flinch from repeating things that all experts know. Furthermore, I hope and expect that many of the points I ma

智力高

Dimensional and Analytic Renormalization,ain (interacting) field operators evaluated at the space time point x. ε R.. The GellMann Low formula expresses (1.1) as a formal power series whose terms are also time-ordered vacuum expectation values, similar to (1.1), but involving free rather than interacting fields; since we are not interested

Flatus

,Remark on Equivalent Formulations for Bogoliubov’s Method of Renormalization,l be sketched. In Bogoliubov’s approach the propagators are regularized according to Pauli-Villars so that the unrenormalized Feynman integrals become finite. The renormalized Feynman integrals are then formed by subtracting counter terms which are constructed according to certain combinatorial rule

RALES

Gentry

Gauge Field Models, School [2,3]. It turns out that the naive identities, which can be deduced on a very formal ground, expressing in terms of the Green functions the quantum equivalent of the Noether theorem are affected with quantum correction depending on the particular renormalization rules. In some “clever” renor