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Titlebook: Unbounded Non-Commutative Integration; J. P. Jurzak Book 1985 D. Reidel Publishing Company, Dordretch, Holland 1985 Algebra.Topologie.calc

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書(shū)目名稱(chēng)Unbounded Non-Commutative Integration
編輯J. P. Jurzak
視頻videohttp://file.papertrans.cn/942/941050/941050.mp4
叢書(shū)名稱(chēng)Mathematical Physics Studies
圖書(shū)封面Titlebook: Unbounded Non-Commutative Integration;  J. P. Jurzak Book 1985 D. Reidel Publishing Company, Dordretch, Holland 1985 Algebra.Topologie.calc
描述Non-commutative integration has its origin in the classical papers of Murray and von Neumann on rings of operators, and was introduced because of unsolved problems in unitary group representations and the elucidation of various aspects of quantum-mechanical formalism, together with formal calculus in such operator rings. These papers emphasized the interest in 1I -factors and pOinted out the remarkable behavior and 1 algebraic structure of the set of all unbounded closed operators a. ffiliated to such rings. The absence of power tools in functional analysis - mainly settled in their definitive form by A. Grothendieck around 1950-195- together with the pathological manipulation of algebraic operations on closed operators in Hilbert spaces, has limited ring-theory to the study of algebras of bounded operators with the main objective the difficult question of classifica- tion up to isomorphisms of factors. This material has permitted a rigorous study of discrete systems in statistical mechanics but appears to be less convincing in other domains of physics (in the algebraic approach to field theory, for example). The striking role of Hamiltonians, Schrodinger operators and Lie group in
出版日期Book 1985
關(guān)鍵詞Algebra; Topologie; calculus; field theory; functional analysis; mechanics; operator; statistical mechanics
版次1
doihttps://doi.org/10.1007/978-94-009-5231-7
isbn_softcover978-94-010-8813-8
isbn_ebook978-94-009-5231-7Series ISSN 0921-3767 Series E-ISSN 2352-3905
issn_series 0921-3767
copyrightD. Reidel Publishing Company, Dordretch, Holland 1985
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-Invariance and ,-Traces,Neumann algebra (denoted always by P) generated by all A. and the center Z of M, we get a slightly different definition of .-invariance (with coincidence of both notions for a normal f . 0) and nothing is changed. Such a choice of P has to be taken in definition 9.2.
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Technical Properties of the Domain,rhood V of zero such that, for every ? > 0, there exists a bounded set M. in E satisfying V ? ?U + M.. In particular, it is easily seen that every subspace A ? B (., .) with A = A*, endowed with topology ρ, is quasi-normable.
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Gelfand Transformation,s (.,‖ ‖A..), i ∈ . are Banach spaces: it follows that . is an abelian ? *-algebra containing Id, and consists of operators sending D into itself. Let .’. be the Banach space dual of the ?* -algebra . and K be the spectrum (i.e., the set of characters) of .’ which is known to be compact for σ (.’.,
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Cofinal Central Systems and Derivations, ā. (H) by hypothesis), such that the center of M. contains all ā.. Then it is clear that M. ? L (.), and it follows that . = U. M.A. × A. is a ?-algebra, with natural domain . satisfying condition I, with all A. as a cofinal central system.
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-Invariance and ,-Traces,be ultraweakly closed, satisfying condition II, with a cofinal sequence A., and let M be the von Neumann algebra .. We denote by P the abelian von Neumann algebra generated by all A. and by P. the group of unitary operators of P. Let . be the group of automorphisms of M of the form B ∈ M?U B U. ∈ M,
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