English

Explicit and Almost Explicit Spectral Calculations for Diffusion Operators

Spectral Theory 2008-08-25 v1 Probability

Abstract

The diffusion operator HD=12ddxaddxbddx=12exp(2B)ddxaexp(2B)ddx, H_D=-\frac12\frac d{dx}a\frac d{dx}-b\frac d{dx}=-\frac12\exp(-2B)\frac d{dx}a\exp(2B)\frac d{dx}, where B(x)=0xba(y)dyB(x)=\int_0^x\frac ba(y)dy, defined either on R+=(0,)R^+=(0,\infty) with the Dirichlet boundary condition at x=0x=0, or on RR, can be realized as a self-adjoint operator with respect to the density exp(2Q(x))dx\exp(2Q(x))dx. The operator is unitarily equivalent to the Schr\"odinger-type operator HS=12ddxaddx+Vb,aH_S=-\frac12\frac d{dx}a\frac d{dx}+V_{b,a}, where Vb,a=12(b2a+b)V_{b,a}=\frac12(\frac{b^2}a+b'). We obtain an explicit criterion for the existence of a compact resolvent and explicit formulas up to the multiplicative constant 4 for the infimum of the spectrum and for the infimum of the essential spectrum for these operators. We give some applications which show in particular how infσ(HD)\inf\sigma(H_D) scales when a=νa0a=\nu a_0 and b=γb0b=\gamma b_0, where ν\nu and γ\gamma are parameters, and a0a_0 and b0b_0 are chosen from certain classes of functions. We also give applications to self-adjoint, multi-dimensional diffusion operators.

Keywords

Cite

@article{arxiv.0808.3044,
  title  = {Explicit and Almost Explicit Spectral Calculations for Diffusion Operators},
  author = {Ross G. Pinsky},
  journal= {arXiv preprint arXiv:0808.3044},
  year   = {2008}
}
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