Isbn: 9786131245145 - state (functional analysis): functional analysis, c*-algebra, positive linear functional, operator norm, convex set, probability measure (4 resultados)

ISBN
Refinar con la Búsqueda avanzada

Filtrar la búsqueda

  • Libros (4)

  • Nuevo (4)

a

Intervalo de precios personalizado (EUR)

a

  • Idioma: Inglés

    Editorial: Omniscriptum Mär 2026, 2026

    6131245142 / 9786131245145

    • Tapa blanda
    • Firmado
    • Impresión bajo demanda

    Librería: BuchWeltWeit Ludwig Meier e.K., Bergisch Gladbach, AlemaniaBuchWeltWeit Ludwig Meier e.K.

    Vendedor de 5 estrellas
    Contactar con el vendedor

    Condición: Nuevo

    EUR 34,00

    Envío por EUR 23,00 
    Se envía de Alemania a Estados Unidos de America

    Cantidad disponible: 2 disponibles

    Taschenbuch. Condición: Neu. This item is printed on demand - it takes 3-4 days longer - Neuware -Please note that the content of this book primarily consists of articles available from Wikipedia or other free sources online. In functional analysis, a state on a C -algebra is a positive linear functional of norm 1. The set of states of a C -algebra A, sometimes denoted by S(A), is always a convex set. The extremal points of S(A) are called pure states. If A has a multiplicative identity, S(A) is compact in the weak -topology. In the C -algebraic formulation of quantum mechanics, states in this previous sense correspond to physical states, i.e. mappings from physical observables to their expected measurement outcome.States can be viewed as noncommutative generalizations of probability measures. By Gelfand representation, every commutative C -algebra A is of the form C0(X) for some locally compact Hausdorff X. In this case, S(A) consists of positive Radon measures on X, and the pure states are the evaluation functionals on X. A bounded linear functional on a C -algebra A is said to be self-adjoint if it is real-valued on the self-adjoint elements of A. Self-adjoint functionals are noncommutative analogues of signed measures. 80 pp. Englisch.

  • Idioma: Inglés

    Editorial: OmniScriptum, 2026

    6131245142 / 9786131245145

    • Tapa blanda
    • Impresión bajo demanda

    Librería: preigu, Osnabrück, Alemaniapreigu

    Vendedor de 5 estrellas
    Contactar con el vendedor

    Condición: Nuevo

    EUR 109,85

    Envío por EUR 70,00 
    Se envía de Alemania a Estados Unidos de America

    Cantidad disponible: 5 disponibles

    Taschenbuch. Condición: Neu. State (Functional Analysis) | Functional Analysis, C*-Algebra, Positive Linear Functional, Operator Norm, Convex Set, Probability Measure | Lambert M. Surhone (u. a.) | Taschenbuch | Englisch | 2026 | OmniScriptum | EAN 9786131245145 | Verantwortliche Person für die EU: preigu GmbH & Co. KG, Lengericher Landstr. 19, 49078 Osnabrück, mail[at]preigu[dot]de | Anbieter: preigu Print on Demand.

  • Idioma: Inglés

    Editorial: Omniscriptum Mär 2026, 2026

    6131245142 / 9786131245145

    • Tapa blanda
    • Firmado
    • Impresión bajo demanda

    Librería: buchversandmimpf2000, Emtmannsberg, BAYE, Alemaniabuchversandmimpf2000

    Vendedor de 5 estrellas
    Contactar con el vendedor

    Condición: Nuevo

    EUR 136,00

    Envío por EUR 60,00 
    Se envía de Alemania a Estados Unidos de America

    Cantidad disponible: 1 disponibles

    Taschenbuch. Condición: Neu. This item is printed on demand - Print on Demand Titel. Neuware -Please note that the content of this book primarily consists of articlesavailable from Wikipedia or other free sources online. In functionalanalysis, a state on a C\*-algebra is a positive linear functional ofnorm 1. The set of states of a C\*-algebra A, sometimes denoted by S(A)is always a convex set. The extremal points of S(A) are called purestates. If A has a multiplicative identity, S(A) is compact in theweak\*-topology. In the C\*-algebraic formulation of quantum mechanicsstates in this previous sense correspond to physical states, i.e.mappings from physical observables to their expected measurementoutcome.States can be viewed as noncommutative generalizations ofprobability measures. By Gelfand representation, every commutativeC\*-algebra A is of the form C0(X) for some locally compact Hausdorff X.In this case, S(A) consists of positive Radon measures on X, and thepure states are the evaluation functionals on X. A bounded linearfunctional on a C\*-algebra A is said to be self-adjoint if it isreal-valued on the self-adjoint elements of A. Self-adjoint functionalsare noncommutative analogues of signed measures.VDM Verlag, Dudweiler Landstraße 99, 66123 Saarbrücken 80 pp. Englisch.

  • Idioma: Inglés

    Editorial: Omniscriptum, 2026

    6131245142 / 9786131245145

    • Tapa blanda
    • Impresión bajo demanda

    Librería: AHA-BUCH GmbH, Einbeck, AlemaniaAHA-BUCH GmbH

    Vendedor de 5 estrellas
    Contactar con el vendedor

    Condición: Nuevo

    EUR 189,66

    Envío por EUR 30,50 
    Se envía de Alemania a Estados Unidos de America

    Cantidad disponible: 1 disponibles

    Taschenbuch. Condición: Neu. nach der Bestellung gedruckt Neuware - Printed after ordering - Please note that the content of this book primarily consists of articles available from Wikipedia or other free sources online. In functional analysis, a state on a C -algebra is a positive linear functional of norm 1. The set of states of a C -algebra A, sometimes denoted by S(A), is always a convex set. The extremal points of S(A) are called pure states. If A has a multiplicative identity, S(A) is compact in the weak -topology. In the C -algebraic formulation of quantum mechanics, states in this previous sense correspond to physical states, i.e. mappings from physical observables to their expected measurement outcome.States can be viewed as noncommutative generalizations of probability measures. By Gelfand representation, every commutative C -algebra A is of the form C0(X) for some locally compact Hausdorff X. In this case, S(A) consists of positive Radon measures on X, and the pure states are the evaluation functionals on X. A bounded linear functional on a C -algebra A is said to be self-adjoint if it is real-valued on the self-adjoint elements of A. Self-adjoint functionals are noncommutative analogues of signed measures.