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Alexander K. Motovilov

Publications and source records attributed to Alexander K. Motovilov.

At least 19 recordsLinked to original sources

Two-fermion lattice Hamiltonian with first and second nearest-neighboring-site interactions

We study the Schroedinger operators H_{λμ}(K), with K \in T_2 the fixed quasi-momentum of the particles pair, associated with a system of two identical fermions on the two-dimensional lattice Z_2 with first and second nearest-neighboring-site interactions of magnitudes λ\in R and μ\in R, respectively. We establish a partition of the (λ,μ)-plane so that in each its connected component, the Schroedinger operator H_{λμ}(0) has a definite (fixed) number of eigenvalues, which are situated below the bottom of the essential spectrum and above its top. Moreover, we establish a sharp lower bound for the number of isolated eigenvalues of H_{λμ}(K) in each connected component.

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Optimal bounds on the speed of subspace evolution

By a quantum speed limit one usually understands an estimate on how fast a quantum system can evolve between two distinguishable states. The most known quantum speed limit is given in the form of the celebrated Mandelstam-Tamm inequality that bounds the speed of the evolution of a state in terms of its energy dispersion. In contrast to the basic Mandelstam-Tamm inequality, we are concerned not with a single state but with a (possibly infinite-dimensional) subspace which is subject to the Schroedinger evolution. By using the concept of maximal angle between subspaces we derive optimal bounds on the speed of such a subspace evolution. These bounds may be viewed as further generalizations of the Mandelstam-Tamm inequality. Our study includes the case of unbounded Hamiltonians.

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Quantum speed limits for time evolution of a system subspace

One of the fundamental physical limits on the speed of time evolution of a quantum state is known in the form of the celebrated Mandelstam-Tamm inequality. This inequality gives an answer to the question on how fast an isolated quantum system can evolve from its initial state to an orthogonal one. In its turn, the Fleming bound is an extension of the Mandelstam-Tamm inequality that gives an optimal speed bound for the evolution between non-orthogonal initial and final states. In the present work, we are concerned not with a single state but with a whole (possibly infinite-dimensional) subspace of the system states that are subject to the Schroedinger evolution. By using the concept of maximal angle between subspaces we derive an optimal estimate on the speed of such a subspace evolution that may be viewed as a natural generalization of the Fleming bound.

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Unphysical energy sheets and resonances in the Friedrichs-Faddeev model

We consider the Friedrichs-Faddeev model in the case where the kernel of the potential operator is holomorphic in both arguments on a certain domain of $\mathbb{C}$. For this model we, first, study the structure of the $T$- and $S$-matrices on unphysical energy sheet(s). To this end, we derive representations that explicitly express them in terms of these same operators considered exclusively on the physical sheet. Furthermore, we allow the Friedrichs-Faddeev Hamiltonian undergo a complex deformation (or even a complex scaling/rotation if the model is associated with an infinite interval). Isolated non-real eigenvalues of the deformed Hamiltonian are called the deformation resonances. For a class of perturbation potentials with analytic kernels, we prove that the deformation resonances do correspond to the scattering matrix resonances, that is, they represent the poles of the scattering matrix analytically continued to the respective unphysical sheet.

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Preserving of the unconditional basis property under non-self-adjoint perturbations of self-adjoint operators

Let $T$ be a self-adjoint operator in a Hilbert space $H$ with domain $\mathcal D(T)$. Assume that the spectrum of $T$ is confined in the union of disjoint intervals $Δ_k =[α_{2k-1},α_{2k}]$, $k\in \mathbb{Z}$, and $$ α_{2k+1}-α_{2k} \geq b|α_{2k+1}+α_{2k}|^p\quad \text{ for some }\,b>0,\,p\in[0,1). $$ Suppose that a linear operator $B$ in $H$ is $p$-subordinated to $T$, i.e. $\mathcal D(B) \supset\mathcal D(T)$ and $\|Bx\| \leq b'\,\|Tx\|^p\|x\|^{1-p} +M\|x\| \text{\, for all } x\in \mathcal D(T)$, with some $b'>0$ and $M\geq 0$. Then the spectrum of the perturbed operator $A=T+B$ lies in the union of a rectangle in $\mathbb{C}$ and double parabola $P_{p,h} = \bigl\{λ\in \mathbb{C}\,\bigl|\,|\mathop{\rm Im} λ|\leq h|\mathop{\rm Re} λ|^p\bigr\}$, provided that $h>b'$. The vertical strips $Ω_k =\{λ\in\mathbb{C}|\,|r_k-{\rm Re}\,λ|\leq δr_k^p\}$, $r_k =(α_{2k}+α_{2k+1})/2$, belong to the resolvent set of $T$, provided that $δ<b -b'$ and $ |k|\geq N$ for $N$ large enough. For $|k|\ge N+1$, denote by $Π_k$ the curvilinear trapezoid formed by the lines ${\rm Re}\,λ= r_{k-1}$, ${\rm Re}\,λ= r_{k}$, and the boundary of the parabola $P_{p,h}$. Assume that $Q_0$ is the Riesz projection corresponding to the (bounded) part of the spectrum of $T$ that lies outside $\bigcup_{|k|\geq N+1}Π_k$. And let $Q_k$, $|k|\ge N+1$, be the Riesz projection for the part of the spectrum of $T$ confined within $Π_k$. Main result of the work consists in proving that the system of the invariant subspaces $Q_k(H)$, $|k|\geq N+1$, together with the invariant subspace $Q_0(H)$ forms an unconditional basis of subspaces in the space $H$.

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Solvability of the operator Riccati equation in the Feshbach case

We consider a bounded block operator matrix of the form $$ L=\left(\begin{array}{cc} A & B \\ C & D \end{array} \right), $$ where the main-diagonal entries $A$ and $D$ are self-adjoint operators on Hilbert spaces $H_{_A}$ and $H_{_D}$, respectively; the coupling $B$ maps $H_{_D}$ to $H_{_A}$ and $C$ is an operator from $H_{_A}$ to $H_{_D}$. It is assumed that the spectrum $σ_{_D}$ of $D$ is absolutely continuous and uniform, being presented by a single band $[α,β]\subset\mathbb{R}$, $α<β$, and the spectrum $σ_{_A}$ of $A$ is embedded into $σ_{_D}$, that is, $σ_{_A}\subset(α,β)$. We formulate conditions under which there are bounded solutions to the operator Riccati equations associated with the complexly deformed block operator matrix $L$; in such a case the deformed operator matrix $L$ admits a block diagonalization. The same conditions also ensure the Markus-Matsaev-type factorization of the Schur complement $M_{_A}(z)=A-z-B(D-z)^{-1}C$ analytically continued onto the unphysical sheet(s) of the complex $z$ plane adjacent to the band $[α,β]$. We prove that the operator roots of the continued Schur complement $M_{_A}$ are explicitly expressed through the respective solutions to the deformed Riccati equations.

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On invariant graph subspaces of a J-self-adjoint operator in the Feshbach case

We consider a J-self-adjoint 2x2 block operator matrix L in the Feshbach spectral case, that is, in the case where the spectrum of one main-diagonal entry is embedded into the absolutely continuous spectrum of the other main-diagonal entry. We work with the analytic continuation of one of the Schur complements of L to the unphysical sheets of the spectral parameter plane. We present the conditions under which the continued Schur complement has operator roots, in the sense of Markus-Matsaev. The operator roots reproduce (parts of) the spectrum of the Schur complement, including the resonances. We then discuss the case where there are no resonances and the associated Riccati equations have bounded solutions allowing the graph representations for the corresponding J-orthogonal invariant subspaces of L. The presentation ends with an explicitly solvable example.

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An alternative proof of the a priori $\tanΘ$ Theorem

Let $A$ be a self-adjoint operator in a separable Hilbert space. Suppose that the spectrum of $A$ is formed of two isolated components $σ_0$ and $σ_1$ such that the set $σ_0$ lies in a finite gap of the set $σ_1$. Assume that $V$ is a bounded additive self-adjoint perturbation of $A$, off-diagonal with respect to the partition ${\rm spec}(A)=σ_0 \cup σ_1$. It is known that if $\|V\|<\sqrt{2}{\rm dist}(σ_0,σ_1)$, then the spectrum of the perturbed operator $L=A+V$ consists of two disjoint parts $ω_0$ and $ω_1$ which originate from the corresponding initial spectral subsets $σ_0$ and $σ_1$. Moreover, for the difference of the spectral projections $E_A(σ_0)$ and $E_{L}(ω_0)$ of $A$ and $L$ associated with the spectral sets $σ_0$ and $ω_0$, respectively, the following sharp norm bound holds: $$\|E_A(σ_0)-E_{L}(ω_0)\|\leq\sin\left(\arctan\frac{\|V\|}{{\rm dist}(σ_0,σ_1)}\right).$$ In the present note, we give a new proof of this bound for $\|V\|<{\rm dist}(σ_0,σ_1)$.

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Bounds on variation of the spectrum and spectral subspaces of a few-body Hamiltonian

We overview the recent results on the shift of the spectrum and norm bounds for variation of spectral subspaces of a Hermitian operator under an additive Hermitian perturbation. Along with the known results, we present a new subspace variation bound for the generic off-diagonal subspace perturbation problem. We also demonstrate how some of the abstract results may work for few-body Hamiltonians.

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Comment on `The tan θ theorem with relaxed conditions', by Y. Nakatsukasa

We show that in case of the spectral norm, one of the main results of the recent paper "The tan θ theorem with relaxed conditions", by Yuji Nakatsukasa, published in Linear Algebra and its Applications is a corollary of the tan θ theorem proven in [V.Kostrykin, K.A.Makarov, and A.K.Motovilov, On the existence of solutions to the operator Riccati equation and the tan θ theorem, IEOT 51 (2005), 121-140]. We also give an alternative finite-dimensional matrix formulation of another tan θ theorem proven in [S.Albeverio and A.K.Motovilov, The a priori tan θ theorem for spectral subspaces, IEOT 73 (2012), 413-430].

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Sharpening the norm bound in the subspace perturbation theory

Let A be a self-adjoint operator on a Hilbert space H. Assume that σ is an isolated component of the spectrum of A, i.e. dist(σ,Σ)=d>0 where Σ=spec(A)\σ. Suppose that V is a bounded self-adjoint operator on H such that ||V|| R^+, that is essentially stronger than the previously known estimates for ||P-Q||. In particular, the bound obtained ensures that ||P-Q||<1 and, thus, that the spectral subspaces Ran(P) and Ran(Q) are in the acute-angle case whenever ||V||<cd with c=0.454169... (the precise expression for c is also given). Our proof of the above results is based on using the triangle inequality for the maximal angle between subspaces and on employing the a priori generic \sin2θestimate for the variation of a spectral subspace. As an example, the boundedly perturbed quantum harmonic oscillator is discussed.

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The a priori Tan Theta Theorem for spectral subspaces

Let A be a self-adjoint operator on a separable Hilbert space H. Assume that the spectrum of A consists of two disjoint components s_0 and s_1 such that the set s_0 lies in a finite gap of the set s_1. Let V be a bounded self-adjoint operator on H off-diagonal with respect to the partition spec(A)=s_0 \cup s_1. It is known that if ||V||<\sqrt{2}d, where d=\dist(s_0,s_1), then the perturbation V does not close the gaps between s_0 and s_1 and the spectrum of the perturbed operator L=A+V consists of two isolated components s'_0 and s'_1 grown from s_0 and s_1, respectively. Furthermore, it is known that if V satisfies the stronger bound ||V||< d then the following sharp norm estimate holds: ||E_L(s'_0)-E_A(s_0)|| \leq sin(arctan(||V||/d)), where E_A(s_0) and E_L(s'_0) are the spectral projections of A and L associated with the spectral sets s_0 and s'_0, respectively. In the present work we prove that this estimate remains valid and sharp also for d \leq ||V||< \sqrt{2}d, which completely settles the issue.

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Bounds on the spectrum and reducing subspaces of a J-self-adjoint operator

Given a self-adjoint involution J on a Hilbert space H, we consider a J-self-adjoint operator L=A+V on H where A is a possibly unbounded self-adjoint operator commuting with J and V a bounded J-self-adjoint operator anti-commuting with J. We establish optimal estimates on the position of the spectrum of L with respect to the spectrum of A and we obtain norm bounds on the operator angles between maximal uniformly definite reducing subspaces of the unperturbed operator A and the perturbed operator L. All the bounds are given in terms of the norm of V and the distances between pairs of disjoint spectral sets associated with the operator L and/or the operator A. As an example, the quantum harmonic oscillator under a PT-symmetric perturbation is discussed. The sharp norm bounds obtained for the operator angles generalize the celebrated Davis-Kahan trigonometric theorems to the case of J-self-adjoint perturbations.

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Progress in methods to solve the Faddeev and Yakubovsky differential equations

We shortly recall the derivation of the Faddeev-Yakubovsky differential equations and point out their main advantages. Then we give a review of the numerical approaches used to solve the bound-state and scattering problems for the three- and four-body systems based on these equations. A particular attention is payed to the latest developments.

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Perturbation of spectra and spectral subspaces

We consider the problem of variation of spectral subspaces for linear self-adjoint operators under off-diagonal perturbations. We prove a number of new optimal results on the shift of the spectrum and obtain (sharp) estimates on the norm of the difference of two spectral projections.

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