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Keisuke Asahara

Publications and source records attributed to Keisuke Asahara.

4 recordsLinked to original sources

Two-dimensional quantum central limit theorem by quantum walks

The weak limit theorem (WLT), the quantum analogue of the central limit theorem, is foundational to quantum walk (QW) theory. Unlike the universal Gaussian limit of classical walks, deriving analytical forms of the limiting probability density function (PDF) in higher dimensions has remained a challenge since the 1D Konno distribution was established. Previous explicit PDFs for 2D models were limited to specific cases whose fundamental nature was unclear. This paper resolves this long-standing gap by introducing the notion of maximal speed $v_{\mathrm{max}}$ as a critical parameter. We demonstrate that all previous 2D solutions correspond to a degenerate regime where $v_{\mathrm{max}} = 1$. We then present the first exact analytical representation of the limiting PDF for the physically richer, unexplored regime $v_{\mathrm{max}} < 1$ of a general class of 2D two-state QWs. Our result reveals 2D Konno functions that govern these dynamics. We establish these as the proper 2D generalization of the 1D Konno distribution by demonstrating their convergence to the 1D form in the appropriate limit. Furthermore, our derivation, based on spectral analysis of the group velocity map, analytically resolves the singular asymptotic structure: we explicitly determine the caustics loci where the PDF diverges and prove they define the boundaries of the distribution's support. By also providing a closed-form expression for the weight functions, this work offers a complete description of the 2D WLT.

math-ph

Spectral mapping theorem of an abstract non-unitary quantum walk

This paper continues the previous work (Quantum Inf. Process (2019)) by two authors of the present paper about a spectral mapping property of chiral symmetric unitary operators. In physics, they treat non-unitary time-evolution operators to consider quantum walks in open systems. In this paper, we generalize the above result to include a chiral symmetric non-unitary operator whose coin operator only has two eigenvalues. As a result, the spectra of such non-unitary operators are included in the (possibly non-unit) circle and the real axis in the complex plane. We also give some examples of our abstract results, such as non-unitary quantum walks defined by Mochizuki et al. Moreover, we present an application to the Ihara zeta functions and correlated random walks on regular graphs, which are not quantum walks.

math-ph

The Witten Index for One-dimensional Non-unitary Quantum Walks with Gapless Time-evolution

Recent developments in the index theory of discrete-time quantum walks allow us to assign a certain well-defined supersymmetric index to a pair of a unitary time-evolution $U$ and a $\mathbb{Z}_2$-grading operator $\varGamma$ satisfying the chiral symmetry condition $U^* = \varGamma U \varGamma.$ In this paper, this index theory will be extended to encompass non-unitary $U$. The existing literature for unitary $U$ makes use of the indispensable assumption that $U$ is essentially gapped; that is, we require that the essential spectrum of $U$ contains neither $-1$ nor $+1$ to define the associated index. It turns out that this assumption is no longer necessary, if the given time-evolution $U$ is non-unitary. As a concrete example, we shall consider a well-known non-unitary quantum walk model on the one-dimensional integer lattice, introduced by Mochizuki-Kim-Obuse.

math-ph

Spectral analysis of an abstract pair interaction model

We consider an abstract pair-interaction model in quantum field theory with a coupling constant $λ\in {\mathbb R}$ and analyze the Hamiltonian $H(λ)$ of the model. In the massive case, there exist constants $λ_{\rm c}<0$ and $λ_{{\rm c},0}<λ_{\rm c}$ such that, for each $λ\in (λ_{{\rm c},0},λ_{\rm c})\cup (λ_{\rm c},\infty)$, $H(λ)$ is diagonalized by a proper Bogoliubov transformation, so that the spectrum of $H(λ)$ is explicitly identified, where the spectrum of $H(λ)$ for $λ>λ_{\rm c}$ is different from that for $λ\in (λ_{{\rm c},0}, λ_{\rm c})$. As for the case $λ<λ_{{\rm c},0}$, we show that $H(λ)$ is unbounded from above and below. In the massless case, $λ_{\rm c}$ coincides with $λ_{{\rm c},0}$.

math-ph