English

Uncertainty principle and geometry of the infinite Grassmann manifold

Functional Analysis 2017-01-16 v1

Abstract

We study the pairs of projections PIf=χIf,  QJf=(χJf^) ˇ,  fL2(Rn), P_If=\chi_If ,\ \ Q_Jf= \left(\chi_J \hat{f}\right)\check{\ } , \ \ f\in L^2(\mathbb{R}^n), where I,JRnI, J\subset \mathbb{R}^n are sets of finite Lebesgue measure, χI,χJ\chi_I, \chi_J denote the corresponding characteristic functions and  ^, ˇ\hat{\ } , \check{\ } denote the Fourier-Plancherel transformation L2(Rn)L2(Rn)L^2(\mathbb{R}^n)\to L^2(\mathbb{R}^n) and its inverse. These pairs of projections have been widely studied by several authors in connection with the mathematical formulation of Heisenberg's uncertainty principle. Our study is done from a differential geometric point of view. We apply known results on the Finsler geometry of the Grassmann manifold P(H){\cal P}({\cal H}) of a Hilbert space H{\cal H} to establish that there exists a unique minimal geodesic of P(H){\cal P}({\cal H}), which is a curve of the form δ(t)=eitXI,JPIeitXI,J \delta(t)=e^{itX_{I,J}}P_Ie^{-itX_{I,J}} which joins PIP_I and QJQ_J and has length π/2\pi/2. As a consequence we obtain that if HH is the logarithm of the Fourier-Plancherel map, then [H,PI]π/2. \|[H,P_I]\|\ge \pi/2. The spectrum of XI,JX_{I,J} is denumerable and symmetric with respect to the origin, it has a smallest positive eigenvalue γ(XI,J)\gamma(X_{I,J}) which satisfies cos(γ(XI,J))=PIQJ. \cos(\gamma(X_{I,J}))=\|P_IQ_J\|.

Keywords

Cite

@article{arxiv.1701.03733,
  title  = {Uncertainty principle and geometry of the infinite Grassmann manifold},
  author = {Esteban Andruchow and Gustavo Corach},
  journal= {arXiv preprint arXiv:1701.03733},
  year   = {2017}
}