Hydrogen atom on curved noncommutative space

preprint2013arXivOpen access

Abstract

We have calculated the hydrogen atom spectrum on curved noncommutative space defined by the commutation relations [x^i,x^j]=iθω^ij(x^)\left[ \hat {x}^{i},\hat{x}^{j}\right] =iθ\hatω^{ij}\left( \hat {x}\right) , where θθ is the parameter of noncommutativity. The external antisymmetric field which determines the noncommutativity is chosen as ωij(x)=εijkxkf(xixi)ω^{ij}(x) =\varepsilon^{ijk}{x}_{k}f\left( {x_i}x^{i}\right) . In this case the rotational symmetry of the system is conserved, preserving the degeneracy of the energy spectrum. The contribution of the noncommutativity appears as a correction to the fine structure. The corresponding nonlocality is calculated: ΔxΔy≥θ24∣m⟨f2⟩∣ΔxΔy \geq \frac{θ^2}{4} |m\langle f^2\rangle| , where mm is a magnetic quantum number.

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