SearcharxivSearch

arXiv subjects

Abdelkader Intissar

Publications and source records attributed to Abdelkader Intissar.

13 recordsLinked to original sources

New Spectral Properties of Imaginary part of Gribov-Intissar Operator

In 1998, we have given in ([14] Intissar, A., Analyse de Scattering d'un opérateur cubique de Heun dans l'espace de Bargmann, Comm.Math.Phys.199 (1998) 243-256) the boundary conditions at infinity for a description of all maximal dissipative extensions in Bargmann space of the minimal Heun's operator $H_I = z(\frac{d}{dz} + z)\frac{d}{dz}$; $z \in \mathbb{C}$. The characteristic functions of the dissipative extensions have computed and some completeness theorems have obtained for the system of generalized eigenvectors. In ([18] Intissar, A, Le Bellac, M. and Zerner, M., Properties of the Hamiltonian of Reggeon field theory, Phys. Lett. B 113 (1982) 487-489) the non self-adjoint operator $λH_{I}$ where $λ\in \mathbb{R}$ is imaginary part of the Hamiltonian of Reggeon field theory: $$H_{μ, λ} = μz\frac{d}{dz} + i λz( \frac{d}{dz} + z)\frac{d}{dz} \,\, \text{where} \,\, (μ, λ) \in \mathbb{R}^{2} \,\, \text{and} \,\, i^{2} = -1$$ The main purpose of the present work is to present some new spectral properties of right inverse $K_{0, λ}$ of $H_λ = iλH_I$ ($H_λK_{0, λ} = I$) on negative imaginary axis and to study the deficiency numbers of the generalized Heun's operator $H^{p,m} = z^{p}( \frac{d^{m}}{dz^{m}} + z^{m})\frac{d^{p}}{dz^{p}}$ $p, m = 1, 2, ....$. In particular, here we find some conditions on the parameters $p$ and $m$ for that $H_{I}^{p,m}$ to be completely indeterminate.It follows from these conditions that $H^{p,m}$ is entire of the type minimal.

math-ph

Spectral analysis of some non-normal operators arising in Reggeon field theory

In this work, we present a complete spectral study of a family of non-normal operators arising in Reggeon field theory. This family of operators is an original example who permit us to discover the recent theory of physical requirement of space-time reflection symmetry (PT symmetry) without losing any of the essential physical features of quantum mechanics [Bender]. Early studies of Reggeon field theory, in the late 1970s led a number of investigators to observe that model cubic quantum-mechanical Hamiltonians might have real eigenvalues [Bower et al]. The study of this family of operators, permit us to discover some fine results of Spectral Theory and Functional Analysis in particular the results connected with completeness of elementary solutions of mathematical physics problems. We use knowledge basics of holomorphic functions of one complex variable and the properties of Hilbert spaces. In this work the knowledge of spectral theory and the functional analysis of standard level is required (see [Kato], [Ghohberg2 et al] and [Markus]). It is also requested to know the basic properties of semigroup theory see for example ([Pazy]).

math-ph

Application of the criterion of Li-Wang to a five dimensional epidemic model of COVID-19. Part I

The dynamics of many epidemic models for infectious diseases that spread in a single host population demonstrate a threshold phenomenon. If the basic reproduction number R0 is below unity, the disease-free equilibrium P0 is globally stable in the feasible region and the disease always dies out. If R0 > 1, a unique endemic equilibrium P? is globally asymptotically stable in the interior of the feasible region and the disease will persist at the endemic equilibrium if it is initially present. In this paper (Part I), we reinvestigate the study of the stability or the non stability of a mathematical Covid-19 model constructed by Nita H. Shah, Ankush H. Suthar and Ekta N. Jayswal. We use a criterion of Li-Wang for stability of matrices [Li-Wang] on the second additive compound matrix associated to their model. In second paper (Part II), In order to control the Covid-19 system, i.e., force the trajectories to go to the equilibria we will add some control parameters with uncertain parameters to stabilize the five-dimensional Covid-19 system studied in this paper. Based on compound matrices theory, we apply in [Intissar] again the criterion of Li-Wang to study the stability of equilibrium points of Covid-19 system with uncertain parameters. In this part II, all sophisticated technical calculations including those in part I are given in appendices.

math.DS

On an application of generalized Jentzsch theorem to Gribov operator in Bargmann space

{\it In Bargmann representation, the reggeon's field theory{\color{blue} [5]} is caracterized by the non symmetrical Gribov operator $\displaystyle{H_{λ',μ,λ} = λ' A^{*^{2}}A^{2} + μA^{*}A + iλA^{*}(A + A^{*})A}$ where $A^{*}$ and $A$ are the creation and annihilation operators; $[A, A^{*}] = I $.\\ $(λ',μ, λ) \in \mathbb{R}^{3}$ are respectively the four coupling, the intercept and the triple coupling of Pomeron and $i^{2} = -1$. For $λ' > 0 ,μ> 0$, let $σ(λ',μ) \neq 0$ be the smallest eigenvalue of $H_{λ',μ,λ}$, we show in this paper that $σ(λ',μ)$ is positive, increasing and analytic function on the whole real line with respect to $μ$ and that the spectral radius of $H_{λ',μ,λ}^{-1}$ converges to that of $H_{0,μ,λ}^{-1}$ as $λ'$ goes to zero.\\ The above results can be derived from the method used in ({\color{blue} [2]} Commun. Math. Phys. 93, (1984), p:123-139) by Ando-Zerner to study the smallest eigenvalue $σ(0,μ)$ of $H_{0,μ,λ}$, however as $H_{λ',μ,λ}$ is regular perturbation of $H_{0,μ,λ}$ then its study is much more easily. We can exploit the structure of $H_{λ',μ,λ}^{-1}$ to deduce the results of Ando-Zerner established on the function $σ(0,μ)$ as $λ'$ goes to zero.\\}

math-ph

On the zeros of some families of polynomials satisfying a three-term recurrence associated to Gribov operator

We consider families of tridiagonal- matrices with diagonal $β_{k} = μk$ and off-diagonal entries $α_{k} = iλk\sqrt{k+1}$; $1 \leq k \leq n$, $n \in \mathbb{N}$ and $i^{2} = -1$ where $μ\in \mathbb{C}$ and $λ\in \mathbb{C}$.\\\quad In Gribov theory ([7], A reggeon diagram technique, Soviet Phys. JETP 26 (1968), no. 2, 414-423), the parmeters $μ$ and $λ$ are reals and they are important in the reggeon field theory. In this theory $μ$ is the intercept of Pomeron which describes the energy of dependence of total hadronic cross sections in the currently available range of energies and $λ$ is the triple coupling of Pomeron. The main motive of the paper is the localization of eigenvalues $z_{k,n}(μ, λ)$ of the above matrices which are the zeros of the polynomials $P_{n+1}^{^{μ,λ}}(z)$ satisfying a three-term recurrence : $\left\{\begin{array}[c]{l}P_{0}^{^{μ,λ}}(z) = 0\\\quad\\ P_{1}^{^{μ,λ}}(z) = 1\\\quad \\ α_{n-1}P_{n-1}^{^{μ,λ}}(z) + β_{n}P_{n}^{^{μ,λ}}(z) + α_{n}P_{n+1}^{^{μ,λ}}(z) = zP_{n}^{^{μ,λ}}(z);\quad n\geq 1\\ \end{array} \right. $ \quad \n If $μ\in \mathbb{R}$ and $λ\in \mathbb{R}$ then the above matrices are complex symmetric, in this case we show existence of complex-valued function $ξ(z)$ of bounded variation on $\mathbb{R}$ such that the polynomials $P_{n}^{^{μ,λ}}(z)$ are orthogonal with this weight $ξ(z)$.\\ }

math-ph

On the complete indeterminacy and the chaoticity of generalized operator of Heun in Bargmann space

In Communications in Mathematical Physics, no. 199, (1998), we have considered the Heun operator $\displaystyle{ H = a^* (a + a^*)a}$ acting on Bargmann space where $a$ and $a^{*}$ are the standard Bose annihilation and creation operators satisfying the commutation relation $[a, a^{*}] = I$. We have used the boundary conditions at infinity to give a description of all maximal dissipative extensions in Bargmann space of the minimal Heun's operator $H$. The characteristic functions of the dissipative extensions have be computed and some completeness theorems have be obtained for the system of generalized eigenvectors of this operator. In this paper we study the deficiency numbers of the generalized Heun's operator $\displaystyle{ H^{p,m} = a^{*^{p}} (a^{m} + a^{*^{m}})a^{p}; (p, m=1, 2, .....)}$ acting on Bargmann space. In particular, here we find some conditions on the parameters $p$ and $m$ for that $\displaystyle{ H^{p,m}}$ to be completely indeterminate. It follows from these conditions that $\displaystyle{ H^{p,m}}$ is entire of the type minimal. And we show that $\displaystyle{H^{p,m}}$ and $\displaystyle{ H^{p,m}+ H^{*^{p,m}}}$ (where $H^{*^{p,m}}$ is the adjoint of the $H^{p,m}$) are connected at the chaotic operators. We will give a description of all maximal dissipative extensions and all selfadjoint extensions of the minimal generalized Heun's operator $H^{p,m}$ acting on Bargmann space in separate paper.

math.SP

On regularized trace formula of Gribov semigroup genrated by the Hamiltonian of reggeon field theory in Bargmann representation

In J. Math. Anal. App. 305. (2005), we have considered the Gribov operator\\ $H_{λ'} = λ' S + H_{μ,λ}$ acting on Bargmann space where $ S = a^{*2} a^{2}$ and $ H_{μ,λ} =μa^* a + \ıλa^* (a+a^*)a$ with $i^{2} = -1$.\\ Here $a$ and $a^{*}$ are the standard Bose annihilation and creation operators satisfying the commutation relation $[a, a^{*}] = I$. In Reggeon field theory, the real parameters $λ{'}$ is the four coupling of Pomeron, $μ$ is Pomeron intercept, $λ$ is the triple coupling of Pomeron and $i^{2} = -1$.\\ We have given an approximation of the semigroup $e^{-tH_{λ'}}$ generated by the operator $H_{λ'}$. In particulary, we have obtained an estimate approximation in trace norm of this semigroup by the unperturbed semigroup $e^{-tλ'S}$. In {\bf[12]}, we have regularized the operator $H_{μ,λ}$ by $λ''G$ where $G = a^{*3} a^{3}$, i.e we have considered $H_{λ''} = λ'' G + H_{μ,λ}$ where $λ''$ is the {\it magic coupling} of Pomeron. In this case, we have established an exact relation between the degree of subordination of the non-self-adjoint perturbation operator $H_{μ,λ}$ to the unperturbed operator $G$ and the number of corrections necessary for the existence of finite formula of the regularized trace. The goal of this article consists to study the trace of the semigroup $e^{-tH_{λ''}}$, in particular to give an asymptotic expansion of this trace as $t \rightarrow 0^{+}$.

math.FA

Regularized trace formula of magic Gribov operator on Bargmann space

In this article, we obtain a regularized trace formula for magic Gribov operator\\ $ H = λ{''}G + H_{μ,λ}$ acting on Bargmann space where $$G = a^{*3}a^{3} \quad \quad and \quad \quad H_{μ,λ} = μa^{*}a + iλa^{*}(a + a^{*})a$$ Here $a$ and $a^{*}$ are the standard Bose annihilation and creation operators and in Reggeon field theory, the real parameters $λ{''}$ is the magic coupling of Pomeron, $μ$ is Pomeron intercept, $λ$ is the triple coupling of Pomeron and $i^{2} = -1$. An exact relation is established between the degree of subordination of the perturbation operator $H_{μ,λ}$ to the unperturbed operator $G$ and the number of corrections necessary for the existence of finite formula of the trace.

math-ph

On chaoticity of the sum of chaotic shifts with their adjoints in Hilbert space and applications to some chaotic weighted shifts acting on some Fock-Bargmann spaces

This article is intended to outline some the recent work by the author on the chaoticity of some specific bakward shift unbounded operators realized as differential operators acting on some Fock-Bargmann spaces and give suficient conditions on a linear unbounded densely defined chaotic shift operator $T$ acting on a Hilbert space for the operator $T+T^*$ to be chaotic where $T^*$ is its adjoint.

math.FA