|  GNS Construction for Observable Algebras | 
Gell-Mann-Naimark-Segal Construction in General {Mostly from an explanation by Abhay, 1985}
  > s.a. observable algebras; operator theory.
  * Idea: A construction used in algebraic
    quantum (field) theory, which allows one to construct, given a star-algebra \(\cal A\) and
    a complex valued "positive" linear functional f defined on it (a state),
    a Hilbert space \(\cal H\) and a representation of the algebra on the Hilbert space.
  $ Construction: If \(\cal A\) is a
    star-algebra, and f : \(\cal A\) → \(\mathbb C\) a "positive"
    (i.e., non-negative) linear functional,
for all A ∈ \(\cal A\), f(A*A) ≥ 0
    (we do not require strict positivity because in many useful physical examples
    we do not have it – f(A) can be the expectation value
    of A in a given state ψ, for example);
  - Define I ⊂ \(\cal A\) as
    I:= {A ∈ \(\cal A\) | f(A*A)
    = 0}; This is a subspace of \(\cal A\), in fact it is a left ideal.
  - Define V:= \(\cal A\)/I
    (so that the inner product will be positive);
  - Then V can be structured as
    an inner product space by defining
\(\langle\){A}, {B}\(\rangle\):= f(A*B), for all A, B ∈ \(\cal A\)
    (and, if we complete it in the standard way, it becomes a Hilbert space);
  - Also, \(\cal A\) acts naturally an
    V by B({A}):= {BA} (if we get the Hilbert space
    by completing V, these operators will in general not be defined
    on the whole \(\cal H\)).
  * Useful result: If \(\cal H\) is a Hilbert
    space with a cyclic representation of a star-algebra \(\cal A\), i.e., one such that
∃ ψ0 ∈ \(\cal H\) such that (for all ψ ∈ \(\cal H\), ∃ A ∈ \(\cal A\) such that ψ = A ψ0) ,
    then this representation is unitarily equivalent to the one obtained by the GNS
    construction, with f(A):= \(\langle\)ψ0,
    Aψ0\(\rangle\).
  > Online resources: see Wikipedia
    page.
References > s.a. entanglement;
  holonomy.
  @ General: Reed in(70);
    Iguri & Castagnino JMP(08)-a0711 [for topological *-algebras];
    Chruściński & Marmo OSID(09)-a0810 [geometric description].
  @ Deformed algebras: Bordemann & Waldmann CMP(98)qa/96;
    Waldmann RPMP(01)m.QA/00;
    Gozzi & Reuter IJMPA(94)ht/03.
  @ Other generalizations: Hofmann CMP(98);
    Naudts & Kuna JPA(01)mp/00 [covariance systems];
    Cariñena et al TMP(07)mp [alternative].
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