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R. Jursenas

Publications and source records attributed to R. Jursenas.

3 recordsLinked to original sources

Weyl families of transformed boundary pairs

Let $(\mathfrak{L},Γ)$ be an isometric boundary pair associated with a closed symmetric linear relation $T$ in a Krein space $\mathfrak{H}$. Let $M_Γ$ be the Weyl family corresponding to $(\mathfrak{L},Γ)$. We cope with two main topics. First, since $M_Γ$ need not be (generalized) Nevanlinna, the characterization of the closure and the adjoint of a linear relation $M_Γ(z)$, for some $z\in\mathbb{C}\smallsetminus\mathbb{R}$, becomes a nontrivial task. Regarding $M_Γ(z)$ as the (Shmul'yan) transform of $zI$ induced by $Γ$, we give conditions for the equality in $\overline{M_Γ(z)}\subseteq\overline{M_{\overlineΓ}(z)}$ to hold and we compute the adjoint $M_{\overlineΓ}(z)^*$. As an application we ask when the resolvent set of the main transform associated with a unitary boundary pair for $T^+$ is nonempty. Based on the criterion for the closeness of $M_Γ(z)$ we give a sufficient condition for the answer. It follows, for example, that, if $T$ is a standard linear relation in a Pontryagin space then the Weyl family $M_Γ$ corresponding to a boundary relation $Γ$ for $T^+$ is a generalized Nevanlinna family. In the second topic we characterize the transformed boundary pair $(\mathfrak{L}^\prime,Γ^\prime)$ with its Weyl family $M_{Γ^\prime}$. The transformation scheme is either $Γ^\prime=ΓV^{-1}$ or $Γ^\prime=VΓ$ with suitable linear relations $V$. Results in this direction include but are not limited to: a 1-1 correspondence between $(\mathfrak{L},Γ)$ and $(\mathfrak{L}^\prime,Γ^\prime)$; the formula for $M_{Γ^\prime}-M_Γ$, for an ordinary boundary triple and a standard unitary operator $V$; construction of a quasi boundary triple from an isometric boundary triple $(\mathfrak{L},Γ_0,Γ_1)$ with $\kerΓ=T$ and $T_0=T^*_0$.

math.FA

The transformation of irreducible tensor operators under spherical functions

The irreducible tensor operators and their tensor products employing Racah algebra are studied. Transformation procedure of the coordinate system operators act on are introduced. The rotation matrices and their parametrization by the spherical coordinates of vector in the fixed and rotated coordinate systems are determined. A new way of calculation of the irreducible coupled tensor product matrix elements is suggested. As an example, the proposed technique is applied for the matrix element construction for two electrons in a field of a fixed nucleus.

math-ph

Development of algebraic techniques for the atomic open-shell MBPT(3)

The atomic third-order open-shell many-body perturbation theory is developed. Special attention is paid to the generation and algebraic analysis of terms of the wave operator and the effective Hamiltonian as well. Making use of occupation-number representation and intermediate normalization, the third-order deviations are worked out by employing a computational software program that embodies the generalized Bloch equation. We prove that in the most general case, the terms of effective interaction operator on the proposed complete model space are generated by not more than eight types of the $n$-body ($n\geq2$) parts of the wave operator. To compose the effective Hamiltonian matrix elements handily, the operators are written in irreducible tensor form. We present the reduction scheme in a versatile disposition form, thus it is suited for the coupled-cluster approach.

physics.atom-ph