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Titlebook: Contributions in Mathematical Physics; A Tribute to Gerard S. Twareque Ali,Kalyan B. Sinha Book 2007 Hindustan Book Agency (India) 2007

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https://doi.org/10.1007/978-3-642-45019-8g two manners of the generalization of the fundamental process of diffusion. Such generalization becomes necessary when the mechanism of motion is more complex than in normal diffusion and may involve coherence, spatial restrictions, trapping, and similar features.
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Thoughts about Anomalous Diffusion: Time-Dependent Coefficients versus Memory Functions,g two manners of the generalization of the fundamental process of diffusion. Such generalization becomes necessary when the mechanism of motion is more complex than in normal diffusion and may involve coherence, spatial restrictions, trapping, and similar features.
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Partial *-Algebras, A Tool for the Mathematical Description of Physical Systems,ras, soon became the standard approach to the mathematically rigorous description of physical systems with infinitely many degrees of freedom. Textbooks flourished and, among many authors, Gérard Emch argued forcefully for the new approach [6].
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Physical Applications of Algebras of Unbounded Operators,ed in many details and this analysis produced, up to now, the monographes [32] and [2]. Some physics appeared first in [28] and [31], in the attempt to describe systems with a . (10.) number of degrees of freedom, following some general ideas originally proposed in the famous Haag and Kastler’s paper, [27], on ..
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Infinite Divisibility in Euclidean Quantum Mechanics,gy eigenvalue; such systems are referred to as “simple systems” in this article. In this case, the ground state itself determines the Hamiltonian completely since.,and therefore .(.) — just as much as . itself — can be said to determine all the properties of the system.
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Partial *-Algebras, A Tool for the Mathematical Description of Physical Systems,chanics. The rationale was to free the theory from particular realizations, linked to specific models, and to focus on the basic structure, namely, the algebra of observables and states on it. This more abstract language, exploiting the deep mathematical theories of C*-algebras and von Neumann algeb
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