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Alfredo Uribe

Publications and source records attributed to Alfredo Uribe.

6 recordsLinked to original sources

Asymptotics of the spectral data of perturbed Stark operators in the half-line with mixed boundary conditions

We obtain sharp asymptotic formulas for the eigenvalues and norming constants of Sturm-Liouville operators associated with the differential expression \[ -\frac{d^2}{dx^2} + x + q(x), \quad x\in [0,\infty), \] together with the boundary condition $\varphi'(0) - b\varphi(0) =0$, $b\in\mathbb{R}$, where \[ q\in \left\{ p\in L^2_{\mathbb{R}}(\mathbb{R}_+,(1+x)^r dx) : p'\in L^2_{\mathbb{R}}(\mathbb{R}_+,(1+x)^r dx)\right\} \] with $r>1$.

math.SP

The fast recurrent subspace on an $N$-level quantum energy transport model

The fast recurrent subspace (the biggest support of all invariant states) of a Weak Coupling Limit Type Quantum Markov Semigroup modeling a quantum transport open system of $N$-energy levels is determined. This is achieved by characterizing the structure of all the invariant state and their spectra in terms of a natural generalization of the Discrete Fourier Transform operator. Finally, the attraction domains and long-time behavior of the evolution are studied on hereditary subalgebras where faithful invariant states exist.

math-ph

One-dimensional Stark operators in the half-line

We obtain asymptotic formulas for the spectral data of perturbed Stark operators associated with the differential expression \[ -\frac{d^2}{dx^2} + x + q(x), \quad x\in [0,\infty), \quad q\in L^1(0,\infty), \] and having either Dirichlet or Neumann boundary condition at the origin.

math.SP

The Dirichlet problem for perturbed Stark operators in the half-line

We consider the perturbed Stark operator $H_q\varphi = -\varphi" + x\varphi + q(x)\varphi$, $\varphi(0)=0$, in $L^2(\mathbb{R}_+)$, where $q$ is a real-valued function that belongs to $\mathfrak{A}_r =\left\{ q\in\mathcal{A}_r\cap\text{AC}[0,\infty) : q'\in\mathcal{A}_r\right\}$, where $\mathcal{A}_r = L^2(\mathbb{R}_+,(1+x)^r dx)$ and $r>1$ is arbitrary but fixed. Let $\left\{\lambda_n(q)\right\}_{n=1}^ \infty$ and $\left\{\kappa_n(q)\right\}_{n=1}^ \infty$ be the spectrum and associated set of norming constants of $H_q$. Let $\{a_n\}_{n=1}^\infty$ be the zeros of the Airy function of the first kind, and let $\omega_r:\mathbb{N}\to\mathbb{R}$ be defined by the rule $\omega_r(n) = n^{-1/3}\log^{1/2}n$ if $r\in(1,2)$ and $\omega_r(n) = n^{-1/3}$ if $r\in[2,\infty)$. We prove that $\lambda_n(q) = -a_n + \pi (-a_n)^{-1/2}\int_0^\infty \text{Ai}^2(x+a_n)q(x)dx + O(n^{-1/3}\omega_r^2(n))$ and $\kappa_n(q) = - 2\pi (-a_n)^{-1/2}\int_0^\infty \text{Ai}(x+a_n)\text{Ai}'(x+a_n)q(x)dx + O(\omega_r^3(n))$, uniformly on bounded subsets of $\mathfrak{A}_r$. In order to obtain these asymptotic formulas, we first show that $\lambda_n:\mathcal{A}_r\to\mathbb{R}$ and $\kappa_n:\mathcal{A}_r\to\mathbb{R}$ are real analytic maps.

math.SP