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The spectrum of a Harmonic Oscillator Operator Perturbed by Point Interactions

Spectral Theory 2015-06-22 v1 Mathematical Physics math.MP

Abstract

We consider the operator L=(d/dx)2+x2y+w(x)y,yL2(R) L = - (d/dx)^2 + x^2 y + w(x) y , y \in L^2(\mathbb{R}) , where w(x)=s[δ(xb)δ(x+b)],b0, w(x) = s [ \delta(x - b) - \delta(x + b)], b \neq 0, real, sCs \in \mathbb{C}. This operator has a discrete spectrum: eventually the eigenvalues are simple and λn=(2n+1)+s2(κ(n)/n)+ρ(n)\lambda_n = (2n + 1) + s^2 (\kappa(n) / n) + \rho(n), where κ(n)=12π[(1)n+1sin(2b2n)12sin(4b2n)] \kappa(n) = \frac{1}{2\pi} [(-1)^{n + 1} \sin ( 2 b \sqrt{2n} ) - \frac{1}{2} \sin ( 4 b \sqrt{2n} ) ] and ρ(n)C(logn)/(n3/2) |\rho(n) | \leq C (\log n) / (n^{3/2}) If s=iγs = i \gamma, γ\gamma real, the number T(γ)T(\gamma) of non-real eigenvalues is finite, and T(γ)[C(1+γ)log(e+γ)]2.T(\gamma) \leq [ C (1 + | \gamma |) \log (e + | \gamma |)]^2. The analogue of the above equations is given in the case of any two-point interaction perturbation w(x)=c+δ(xb)+cδ(x+b),c+,cC.w(x) = c_+ \delta(x - b) + c_- \delta(x + b), c_+, c_- \in \mathbb{C}.

Keywords

Cite

@article{arxiv.1407.4153,
  title  = {The spectrum of a Harmonic Oscillator Operator Perturbed by Point Interactions},
  author = {Boris Mityagin},
  journal= {arXiv preprint arXiv:1407.4153},
  year   = {2015}
}

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65 pages