Titlebook: Symposia on Theoretical Physics and Mathematics 8; Lectures presented a Alladi Ramakrishnan (Director of the Institute) Book 1968 Plenum Pr

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,The (π,, 2,) Reactions on Nuclei,he nucleon to have a large momentum inside the nucleus before the absorption process. For a pion at rest this momentum would be 500 MeV/c, and it is known that not many nucleons have such high momenta. In the case of an absorption by a pair of nucleons, on the other hand, energy and momenta are easi

REP

Muon Capture as a Probe for Nuclear Structure,a means of studying the fundamental weak interaction. In particular considerable work has been done both theoretically and experimentally to check the “universal fermi interaction” hypothesis, and to determine the pseudoscalar coupling constant which becomes important in the μ-capture due to a large

Neutropenia

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COLIC

Developments in the Theory of Univalent Functions,s the domain . onto a Schlicht domain, that is, one which is not self-overlapping and contains no branch points. In investigating the properties of analytic functions univalent in a domain . which is simply connected, one usually confines oneself to the case of the unit disc, for, by the Riemann map

Obligatory

interference

Chagrin

Raikov Systems,nvenient account of this work is to be found in Sections 31–33 of Ref. 2. It is still true that the main interest of the subject is due to its bearing on the structure of .(.) and, more generally, of .(.), where . is a locally compact abelian topological group; this structure is far from being fully

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Relativistic Wave Equations for Higher Spin and Their Quantization, matter of my paper presented at the last Matscience symposium.. It is useful to recall here the main steps in this derivation before proceeding to the problem of second quantization. But let us start by enumerating the basic tenets of the philosophy behind equation (1).

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Contributions to the Relativistic Generalization of the Kinetic Theory of Gases and Statistical Meccantly other meaning, namely, its geometrical structure is determined by the gravitational interactions, therefore, the space-time continuum also represents a geometrization of the gravitational field.