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Physica

Creation and annihilation operators in Fock space

Egon Marx

Published Aug 1, 1970• 3 citations
Publisher
DOI
10.1016/0031-8914(70)90026-1

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Fock representations of multicomponent (particularly non-Abelian anyon) commutation relations

Alexei Daletskii, A. A. Kalyuzhnyi, Eugene Lytvynov +1 more

Let $H$ be a separable Hilbert space and $T$ be a self-adjoint bounded linear operator on $H^{\otimes 2}$ with norm $\le1$, satisfying the Yang--Baxter equation. Bo\.zejko and Speicher (1994) proved that the operator $T$ determines a $T$-deformed Fock space $\mathcal F(H)=\bigoplus_{n=0}^\infty\mathcal F_n(H)$. We start with reviewing and extending the known results about the structure of the $n$-particle spaces $\mathcal F_n(H)$ and the commutation relations satisfied by the corresponding creation and annihilation operators acting on $\mathcal F(H)$. We then choose $H=L^2(X\to V)$, the $L^2$-space of $V$-valued functions on $X$. Here $X:=\mathbb R^d$ and $V:=\mathbb C^m$ with $m\ge2$. Furthermore, we assume that the operator $T$ acting on $H^{\otimes 2}=L^2(X^2\to V^{\otimes 2})$ is given by $(Tf^{(2)})(x,y)=C_{x,y}f^{(2)}(y,x)$. Here, for a.a.\ $(x,y)\in X^2$, $C_{x,y}$ is a linear operator on $V^{\otimes 2}$ with norm $\le1$ that satisfies $C_{x,y}^*=C_{y,x}$ and the spectral quantum Yang--Baxter equation. The corresponding creation and annihilation operators describe a multicomponent quantum system. A special choice of the operator-valued function $C_{xy}$ in the case $d=2$ determines non-Abelian anyons (also called plektons). For a multicomponent system, we describe its $T$-deformed Fock space and the available commutation relations satisfied by the corresponding creation and annihilation operators. Finally, we consider several examples of multicomponent quantum systems.

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Generalized boson and fermion operators with a maximal total occupation property

Nedialka I. Stoilova, Joris Van Der Jeugt

Abstract We propose a new generalization of the standard (anti-)commutation relations for creation and annihilation operators of bosons and fermions. These relations preserve the usual symmetry properties of bosons and fermions. Only the standard (anti-)commutator relation involving one creation and one annihilation operator is deformed by introducing fractional coefficients, containing a positive integer parameterp. The Fock space is determined by the classical definition. The new relations are chosen in such a way that the total occupation number in the system has the maximum valuep. From the actions of creation and annihilation operators in the Fock space, a group theoretical framework is determined, and from here the correspondence with known particle statistics is established.

arXiv:2409.14789•Journal of Physics A Mathematical and Theoretical•Sep 6, 2024•0 citations
Let HHH be a separable Hilbert space and TTT be a self-adjoint bounded linear operator on H⊗2H^{\otimes 2}H⊗2 with norm ≤1\le1≤1, satisfying the Yang--Baxter equation. Bo\.zejko and Speicher (1994) proved that the operator TTT determines a TTT-deformed Fock space F(H)=⨁n=0∞Fn(H)\mathcal F(H)=\bigoplus_{n=0}^\infty\mathcal F_n(H)F(H)=⨁n=0∞​Fn​(H). We start with reviewing and extending the known results about the structure of the nnn-particle spaces Fn(H)\mathcal F_n(H)Fn​(H) and the commutation relations satisfied by the corresponding creation and annihilation operators acting on F(H)\mathcal F(H)F(H). We then choose H=L2(X→V)H=L^2(X\to V)H=L2(X→V), the L2L^2L2-space of VVV-valued functions on XXX. Here X:=RdX:=\mathbb R^dX:=Rd and V:=CmV:=\mathbb C^mV:=Cm with m≥2m\ge2m≥2. Furthermore, we assume that the operator TTT acting on H⊗2=L2(X2→V⊗2)H^{\otimes 2}=L^2(X^2\to V^{\otimes 2})H⊗2=L2(X2→V⊗2) is given by (Tf(2))(x,y)=Cx,yf(2)(y,x)(Tf^{(2)})(x,y)=C_{x,y}f^{(2)}(y,x)(Tf(2))(x,y)=Cx,y​f(2)(y,x). Here, for a.a.\ (x,y)∈X2(x,y)\in X^2(x,y)∈X2, Cx,yC_{x,y}Cx,y​ is a linear operator on V⊗2V^{\otimes 2}V⊗2 with norm ≤1\le1≤1 that satisfies Cx,y∗=Cy,xC_{x,y}^*=C_{y,x}Cx,y∗​=Cy,x​ and the spectral quantum Yang--Baxter equation. The corresponding creation and annihilation operators describe a multicomponent quantum system. A special choice of the operator-valued function CxyC_{xy}Cxy​ in the case d=2d=2d=2 determines non-Abelian anyons (also called plektons). For a multicomponent system, we describe its TTT-deformed Fock space and the available commutation relations satisfied by the corresponding creation and annihilation operators. Finally, we consider several examples of multicomponent quantum systems.
Abstract We propose a new generalization of the standard (anti-)commutation relations for creation and annihilation operators of bosons and fermions. These relations preserve the usual symmetry properties of bosons and fermions. Only the standard (anti-)commutator relation involving one creation and one annihilation operator is deformed by introducing fractional coefficients, containing a positive integer parameterp. The Fock space is determined by the classical definition. The new relations are chosen in such a way that the total occupation number in the system has the maximum valuep. From the actions of creation and annihilation operators in the Fock space, a group theoretical framework is determined, and from here the correspondence with known particle statistics is established.