We consider Hilbert space representations of a generalization of canonical com-mutation relations (CCR): [Xj, Xk]: = XjXk ¡XkXj = iΘjkI (j, k = 1, 2,..., 2n), where Xj ’s are elements of an algebra with identity I, i is the imaginary unit, and Θjk is a real number with Θjk = ¡Θkj (j, k = 1,..., 2n). Some basic aspects on Hilbert space representations of the generalized CCR (GCCR) are discussed. We define a Schrödinger type representation of the GCCR by analogy with the usual Schrödinger representation of the CCR with n degrees of freedom. Also we intro-duce a Weyl type representation of the GCCR. The main result of the present paper is a uniqueness theorem on Weyl representations of the GCCR
AbstractLet H be a separable infinite-dimensional complex Hilbert space and let A,B∈B(H), where B(H)...
In models of a quantum harmonic oscillator coupled to a quantum field with a quadratic interaction, ...
By a representation of a C*-algebra A on a Hilbert space H we mean a morphism : A → L(H). After summ...
We consider Hilbert space representations of a generalization of canonical commutation relations (CC...
AbstractWe consider the problem of representing in Hilbert space commutation relations of the form [...
We introduce a concept of singular Bogoliubov transformation on the abstract boson Fock space and co...
We consider a representation of canonical commutation relations (CCR) appearing in a (non-Abelian) ...
Let (T,H) be a weak Weyl representation of the canonical commutation relation (CCR) with one degree ...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom are...
We consider a family of irreducible Weyl representations of canonical commutation relations with inf...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom are...
Tyt. z nagł.References p. 160.Dostępny również w formie drukowanej.ABSTRACT: Tillmann proved that ev...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom a...
A two-dimensional quantum system of a charged particle interacting with a vector potential determine...
We study densely defined unbounded operators acting between different Hilbert spaces. For these, we ...
AbstractLet H be a separable infinite-dimensional complex Hilbert space and let A,B∈B(H), where B(H)...
In models of a quantum harmonic oscillator coupled to a quantum field with a quadratic interaction, ...
By a representation of a C*-algebra A on a Hilbert space H we mean a morphism : A → L(H). After summ...
We consider Hilbert space representations of a generalization of canonical commutation relations (CC...
AbstractWe consider the problem of representing in Hilbert space commutation relations of the form [...
We introduce a concept of singular Bogoliubov transformation on the abstract boson Fock space and co...
We consider a representation of canonical commutation relations (CCR) appearing in a (non-Abelian) ...
Let (T,H) be a weak Weyl representation of the canonical commutation relation (CCR) with one degree ...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom are...
We consider a family of irreducible Weyl representations of canonical commutation relations with inf...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom are...
Tyt. z nagł.References p. 160.Dostępny również w formie drukowanej.ABSTRACT: Tillmann proved that ev...
Weak Weyl representations of the canonical commutation relation (CCR) with one degree of freedom a...
A two-dimensional quantum system of a charged particle interacting with a vector potential determine...
We study densely defined unbounded operators acting between different Hilbert spaces. For these, we ...
AbstractLet H be a separable infinite-dimensional complex Hilbert space and let A,B∈B(H), where B(H)...
In models of a quantum harmonic oscillator coupled to a quantum field with a quadratic interaction, ...
By a representation of a C*-algebra A on a Hilbert space H we mean a morphism : A → L(H). After summ...