The first purpose of this paper is to show a method of constructing a regular biorthogonal pair based on the commutation rule: ab − ba = I for a pair of operators a and b acting on a Hilbert space H with inner product (⋅| ⋅ ). Here, sequences {ϕn} and {ψn} in a Hilbert space H are biorthogonal if (ϕn|ψm) = δnm, n, m = 0, 1, …, and they are regular if both Dϕ ≡ Span{ϕn} and Dψ ≡ Span{ψn} are dense in H. Indeed, the assumptions to construct the regular biorthogonal pair coincide with the definition of pseudo-bosons as originally given in F. Bagarello [“Pseudobosons, Riesz bases, and coherent states,” J. Math. Phys. 51, 023531 (2010)]. Furthermore, we study the connections between the pseudo-bosonic operators a, b, a†, b† and the pseudo-bosonic operators defined by a regular biorthogonal pair ({ϕn}, {ψn}) and an ONB e of H in H. Inoue [“General theory of regular biorthogonal pairs and its physical applications,” e-print arXiv:math-ph/1604.01967]. The second purpose is to define and study the notion of D-pseudo-bosons in F. Bagarello [“More mathematics for pseudo-bosons,” J. Math. Phys. 54, 063512 (2013)] and F. Bagarello [“From self-adjoint to non self-adjoint harmonic oscillators: Physical consequences and mathematical pitfalls,” Phys. Rev. A 88, 032120 (2013)] and give a method of constructing D-pseudo-bosons on some steps. Then it is shown that for any ONB e = {en} in H and any operators T and T−1 in L†(D), we may construct operators A and B satisfying D-pseudo bosons, where D is a dense subspace in a Hilbert space H and L†(D) the set of all linear operators T from D to D such that T*D⊂D, where T* is the adjoint of T. Finally, we give some physical examples of D-pseudo-bosons based on standard bosons by the method of constructing D-pseudo-bosons stated above.
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