General theory of regular biorthogonal pairs and its physical applications

preprint2016arXivOpen access

Abstract

In this paper we introduce a general theory of regular biorthogonal sequences and its physical applications. Biorthogonal sequences {ϕn}\{ ϕ_{n} \} and {ψn}\{ ψ_{n} \} in a Hilbert space H{\cal H} are said to be regular if Span  {ϕn}Span\; \{ ϕ_{n} \} and Span  {ψn}Span\; \{ ψ_{n} \} are dense in H{\cal H}. The first purpose is to show that there exists a non-singular positive self-adjoint operator $T_{\mbox{$f$}}$ in H{\cal H} defined by an ONB $\mbox{$f$} \equiv \{ f_{n} \}$ in H{\cal H} such that $ϕ_{n}=T_{\mbox{$f$}} f_{n}$ and $ψ_{n}= T_{\mbox{$f$}}^{-1} f_{n}$, n=0,1,⋯n=0,1, \cdots, and such an ONB $\mbox{$f$}$ is unique. The second purpose is to define and study the lowering operators $A_{\mbox{$f$}}$ and $B_{\mbox{$f$}}^{\dagger}$, the raising operators $B_{\mbox{$f$}}$ and $A_{\mbox{$f$}}^{\dagger}$, the number operators $N_{\mbox{$f$}}$ and $N_{\mbox{$f$}}^{\dagger}$ determined by the non-singular positive self-adjoint operator $T_{\mbox{$f$}}$. These operators connect with quasi{\it quasi}-hermitian  quantum  mechanics{\it hermitian \; quantum \; mechanics} and its relatives. This paper clarifies and simplifies the mathematical structure of this framework minimized the required assumptions.

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