{"title":"(mathbb{Z}_{2}-)Graded Lie Algebra of Quaternions and Superconformal Algebra in (D=4) Dimensions","authors":"B. C. S. Chauhan, P.K. Joshi, B.C. Chanyal","doi":"10.1134/S106192082402002X","DOIUrl":"10.1134/S106192082402002X","url":null,"abstract":"<p> In the present discussion, we have studied the <span>(mathbb{Z}_{2}-)</span><span>(grading)</span> of the quaternion algebra <span>((mathbb{H}))</span>. We have made an attempt to extend the quaternion Lie algebra to the graded Lie algebra by using the matrix representations of quaternion units. The generalized Jacobi identities of <span>(mathbb{Z}_{2}-graded)</span> algebra then result in symmetric graded partners <span>((N_{1},N_{2},N_{3}))</span>. The graded partner algebra <span>((mathcal{F}))</span> of quaternions <span>((mathbb{H}))</span> thus has been constructed from this complete set of graded partner units <span>((N_{1},N_{2},N_{3}))</span>, and <span>(N_{0}=C)</span>. Keeping in view the algebraic properties of the graded partner algebra <span>((mathcal{F}))</span>, the <span>(mathbb{Z}_{2}-graded)</span> superspace <span>((S^{l,m}))</span> of quaternion algebra <span>((mathbb{H}))</span> has been constructed. It has been shown that the antiunitary quaternionic supergroup <span>(UU_{a}(l;m;mathbb{H}))</span> describes the isometries of <span>(mathbb{Z}_{2}-graded)</span> superspace <span>((S^{l,m}))</span>. The Superconformal algebra in <span>(D=4)</span> dimensions is then established, where the bosonic sector of the Superconformal algebra has been constructed from the quaternion algebra <span>((mathbb{H}))</span> and the fermionic sector from the graded partner algebra <span>((mathcal{F}))</span>: asymmetric space, convex set, <span>(delta)</span>-sun, <span>(gamma)</span>-sun. </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 2","pages":"162 - 176"},"PeriodicalIF":1.7,"publicationDate":"2024-06-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141504356","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Asymptotics of the Solution of the Initial Boundary Value Problem for the One-Dimensional Klein–Gordon Equation with Variable Coefficients","authors":"S.Yu. Dobrokhotov, E.S. Smirnova","doi":"10.1134/S1061920824020043","DOIUrl":"10.1134/S1061920824020043","url":null,"abstract":"<p> In the paper, formal asymptotic solutions of the initial-boundary value problem for the one-dimensional Klein–Gordon equation with variable coefficients on the semi-axis are constructed. Such a problem can be used, in particular, to simulate the propagation of plane acoustic waves in atmospheric gas initiated by a source at the lower boundary of the domain. </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 2","pages":"187 - 198"},"PeriodicalIF":1.7,"publicationDate":"2024-06-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141523511","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Natural Volume Forms on Pseudo-Finslerian Manifolds with (m)th Root Metrics","authors":"A.V. Solov’yov","doi":"10.1134/S1061920824020146","DOIUrl":"10.1134/S1061920824020146","url":null,"abstract":"<p> We define natural volume forms on <span>(n)</span>-dimensional oriented pseudo-Finslerian manifolds with nondegenerate <span>(m)</span>-th root metrics. Our definitions of the natural volume forms depend on the parity of the positive integer <span>(m>1)</span>. The advantage of the stated definitions is their algebraic structure. The natural volume forms are expressed in terms of Cayley hyperdeterminants. In particular, the computation of the natural volume form does not require the difficult integration over the domain within the indicatrix in the tangent space <span>(T_x M^n)</span> of the pseudo-Finslerian manifold at a point <span>(x)</span>. </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 2","pages":"317 - 324"},"PeriodicalIF":1.7,"publicationDate":"2024-06-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141523520","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Probabilistic Bernoulli and Euler Polynomials","authors":"T. Kim, D. S. Kim","doi":"10.1134/S106192084010072","DOIUrl":"10.1134/S106192084010072","url":null,"abstract":"<p> Let <span>(Y)</span> be a random variable whose moment generating function exists in a neighborhood of the origin. The aim of this paper is to introduce and study the probabilistic extension of Bernoulli polynomials and Euler polynomials, namely the probabilistic Bernoulli polynomials associated <span>(Y)</span> and the probabilistic Euler polynomials associated with <span>(Y)</span>. Also, we introduce the probabilistic <span>(r)</span>-Stirling numbers of the second associated <span>(Y)</span>, the probabilistic two variable Fubini polynomials associated <span>(Y)</span>, and the probabilistic poly-Bernoulli polynomials associated with <span>(Y)</span>. We obtain some properties, explicit expressions, certain identities and recurrence relations for those polynomials. As special cases of <span>(Y)</span>, we treat the gamma random variable with parameters <span>(alpha,beta > 0)</span>, the Poisson random variable with parameter <span>(alpha >0)</span>, and the Bernoulli random variable with probability of success <span>(p)</span>. </p><p> <b> DOI</b> 10.1134/S106192084010072 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"94 - 105"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171670","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Another Billiard Problem","authors":"S. Bolotin, D. Treschev","doi":"10.1134/S106192084010047","DOIUrl":"10.1134/S106192084010047","url":null,"abstract":"<p> Let <span>((M,g))</span> be a Riemannian manifold, <span>(Omegasubset M)</span> a domain with boundary <span>(Gamma)</span>, and <span>(phi)</span> a smooth function such that <span>(phi|_Omega > 0)</span>, <span>( varphi |_Gamma = 0)</span>, and <span>(dphi|_Gammane 0)</span>. We study the geodesic flow of the metric <span>(G=g/phi)</span>. The <span>(G)</span>-distance from any point of <span>(Omega)</span> to <span>(Gamma)</span> is finite, hence, the geodesic flow is incomplete. Regularization of the flow in a neighborhood of <span>(Gamma)</span> establishes a natural reflection law from <span>(Gamma)</span>. This leads to a certain (not quite standard) billiard problem in <span>(Omega)</span>. </p><p> <b> DOI</b> 10.1134/S106192084010047 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"50 - 59"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171699","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Piatnitski, V. Sloushch, T. Suslina, E. Zhizhina
{"title":"On the Homogenization of Nonlocal Convolution Type Operators","authors":"A. Piatnitski, V. Sloushch, T. Suslina, E. Zhizhina","doi":"10.1134/S106192084010114","DOIUrl":"10.1134/S106192084010114","url":null,"abstract":"<p> In <span>(L_2(mathbb{R}^d))</span>, we consider a self-adjoint bounded operator <span>({mathbb A}_varepsilon)</span>, <span>(varepsilon >0)</span>, of the form </p><p> It is assumed that <span>(a(mathbf{x}))</span> is a nonnegative function such that <span>(a(-mathbf{x}) = a(mathbf{x}))</span> and <span>(int_{mathbb{R}^d} (1+| mathbf{x} |^4) a(mathbf{x}),dmathbf{x}<infty)</span>; <span>(mu(mathbf{x},mathbf{y}))</span> is <span>(mathbb{Z}^d)</span>-periodic in each variable, <span>(mu(mathbf{x},mathbf{y}) = mu(mathbf{y},mathbf{x}))</span> and <span>(0< mu_- leqslant mu(mathbf{x},mathbf{y}) leqslant mu_+< infty)</span>. For small <span>(varepsilon)</span>, we obtain an approximation of the resolvent <span>(({mathbb A}_varepsilon + I)^{-1})</span> in the operator norm on <span>(L_2(mathbb{R}^d))</span> with an error of order <span>(O(varepsilon^2))</span>. </p><p> <b> DOI</b> 10.1134/S106192084010114 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"137 - 145"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171701","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On Perturbation of Thresholds in Essential Spectrum under Coexistence of Virtual Level and Spectral Singularity","authors":"D.I. Borisov, D.A. Zezyulin","doi":"10.1134/S106192084010059","DOIUrl":"10.1134/S106192084010059","url":null,"abstract":"<p> We study the perturbation of the Schrödinger operator on the plane with a bounded potential of the form <span>(V_1(x)+V_2(y),)</span> where <span>(V_1)</span> is a real function and <span>(V_2)</span> is a compactly supported function. It is assumed that the one-dimensional Schrödinger operator <span>( mathcal{H} _1)</span> with the potential <span>(V_1)</span> has two real isolated eigenvalues <span>( Lambda _0,)</span> <span>( Lambda _1)</span> in the lower part of its spectrum, and the one-dimensional Schrödinger operator <span>( mathcal{H} _2)</span> with the potential <span>(V_2)</span> has a virtual level at the boundary of its essential spectrum, i.e., at <span>(lambda=0)</span>, and a spectral singularity at the inner point of the essential spectrum <span>(lambda=mu>0)</span>. In addition, the eigenvalues and the spectral singularity overlap in the sense of the equality <span>( lambda _0:= Lambda _0+mu= Lambda _1.)</span> We show that a perturbation by an abstract localized operator leads to a bifurcation of the internal threshold <span>( lambda _0)</span> into four spectral objects which are resonances and/or eigenvalues. These objects correspond to the poles of the local meromorphic continuations of the resolvent. The spectral singularity of the operator <span>( mathcal{H} _2)</span> qualitatively changes the structure of these poles as compared to the previously studied case where no spectral singularity was present. This effect is examined in detail, and the asymptotic behavior of the emerging poles and corresponding spectral objects of the perturbed Schrödinger operator is described. </p><p> <b> DOI</b> 10.1134/S106192084010059 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"60 - 78"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171672","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"The (q)-Analog of the Quantum Theory of Angular Momentum: a Review from Special Functions","authors":"R. Álvarez-Nodarse, A. Arenas-Gómez","doi":"10.1134/S106192084010023","DOIUrl":"10.1134/S106192084010023","url":null,"abstract":"<p> In the present paper, we review the <span>(q)</span>-analog of the Quantum Theory of Angular Momentum based on the <span>(q)</span>-algebra <span>(su_q(2))</span> with a special emphasis on the representation of the Clebsch–Gordan coefficients in terms of <span>(q)</span>-hypergeometric series. This representation allows us to obtain several known properties of the Clebsch–Gordan coefficients in an unified and simple way. </p><p> <b> DOI</b> 10.1134/S106192084010023 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"24 - 43"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171663","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"On the Linearization of Certain Singularities of Nijenhuis Operators","authors":"A.Yu. Konyaev","doi":"10.1134/S106192084010084","DOIUrl":"10.1134/S106192084010084","url":null,"abstract":"<p> We consider a linearization problem for Nijenhuis operators in dimension two around a point of scalar type in analytic category. The problem was almost completely solved in [8]. One case, however, namely the case of left-symmetric algebra <span>(mathfrak b_{1, alpha})</span>, proved to be difficult. Here we solve it and, thus, complete the solution of the linearization problem for Nijenhuis operators in dimension two. The problem turns out to be related to classical results on the linearization of vector fields and their monodromy mappings. </p><p> <b> DOI</b> 10.1134/S106192084010084 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"106 - 111"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171700","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Analytical Complexity and Signal Coding","authors":"V.K. Beloshapka","doi":"10.1134/S106192084010035","DOIUrl":"10.1134/S106192084010035","url":null,"abstract":"<p> There are two ways to describe a geometric object <span>(L)</span>: the object as an image of a mapping and the object as a preimage. Every method has its own advantages and shortcomings; together, they give a complete picture. In order to compare these descriptions by complexity, one can use Kolmogorov’s approach: i.e., after the clarification of the system of basic operations, the complexity of a description is the minimum length of the defining text. Accordingly, we obtain two Kolmogorov complexities: in the first case, <span>(K^{+}(L))</span>, and in the other, <span>(K^{-}(L))</span>. Let <span>(Cl^n)</span> be the class of functions of two variables that can be represented by analytic functions of one variable and by the addition of the depth not exceeding <span>(n)</span>, and let <span>(K^{+}(Cl^n))</span> and <span>(K^{-}(Cl^n))</span> be their corresponding Kolmogorov complexities. There are arguments in favor of the fact that, for <span>(n geq 2)</span>, the value of <span>(K^{-}(Cl^n))</span> is very large, and the task of constructing a description of <span>(Cl^n)</span> in the form of a preimage (by defining relations) even for <span>(n=2)</span> is computationally unrealizable. Based on this observation, a signal encoding-decoding scheme is proposed, and arguments are given in favor of the fact that the decoding of a signal encoded using such a scheme is inaccessible to a quantum computer. </p><p> <b> DOI</b> 10.1134/S106192084010035 </p>","PeriodicalId":763,"journal":{"name":"Russian Journal of Mathematical Physics","volume":"31 1","pages":"44 - 49"},"PeriodicalIF":1.7,"publicationDate":"2024-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140171664","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}