By Faddeev L.D.
The behaviour of the analytic components on an infraconnected set D in okay an algebraically closed whole ultrametric box is principally defined by way of the round filters and the monotonous filters on D, particularly the T-filters: zeros of the weather, Mittag-Leffler sequence, factorization, Motzkin factorization, greatest precept, injectivity, algebraic houses of the algebra of the analytic parts on D, difficulties of analytic extension. this is often utilized to the differential equation y'=hy (y,h analytic parts on D), analytic interpolation, p-adic crew duality on meromorphic items and to the p-adic Fourier remodel 1. 30 Years in Mathematical Physics -- 2. Perturbation conception for Gauge-Invariant Fields / V.N. Popov and L. Faddev -- three. The Feynman essential for Singular Lagrangians -- four. Covariant Quantization of the Gravitational box / V.N. Popov and L. Faddev -- five. creation to practical equipment -- 6. Inverse challenge of Quantum Scattering thought. II -- 7. Quantum thoroughly Integrable types in box concept -- eight. The Quantum approach to the Inverse challenge and the Heisenberg XYZ version / L.A. Takhtadzhan and L. Faddev -- nine. Integrable versions in (1+1)-Dimensional Quantum box idea -- 10. From Integrable versions to Conformal box idea through Quantum teams -- eleven. the quest for Multidimensional Solitons -- 12. Hamiltonian method of the idea of Anomalies -- thirteen. The power challenge in Einstein's concept of Gravitation -- 14. Lagrangian Mechanics in Invariant shape / A.M. Vershik and L. Faddev
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1) the factor which is proportional to the orbit volume. 6) where the factors A  or
] aapear, which depend on B in the case of a non-abelian gauge fields. The following will illustrate this procedure on concrete examples. III. QUANTUM ELECTRODYNAMICS This results scheme It is section has a methodological character. Here we show how all known of quantum electrodynamics can be obtained by means of the general of part I. well known that the Lagrangian of electrodynamics: w h e r e « £ f - ^ / < ^ is invarrant wiih respect to the abellan gauge group: The first recipe of Sec.
As an excuse I can claim that when I was studying the one-dimensional Schrodinger equation at the end of the 1950s, I looked on it as an intermediate example between the radial and the three-dimensional equations and directed my attention in the first place to the essential new properties of the scattering matrix that followed from the local property of the potential. However, this problem un expectedly acquired a new meaning in the inverse problem method over a period of 10 years. Apparently unaware of Marchenko's correction, Deift and Trubowitz published a long paper  in 1979 which very dramatically represented the history of my error.
Reported at the Seminar in Institute for Theoretical Physics, Kiev, Ukrainian SSR. •Permanent Address: Mathematical Institute, Leningrad, USSR. 32 214 I. INTRODUCTION It is well known that certain difficulties are involved in the quantization of gauge-invariant fields, and that they are due to the singular nature of the Lagrangian concerned. 1 But this technique does not work in the case of a non-abelian gauge group. 2 He noted, for instance, that diagrams with closed loops depend non-trivially on the ongitudinal parts of Green's functions (in internal lines), and the scattering ampliudes obtained were neither unitary nor transverse.