Abstract
Let H be a self-adjoint operator on a complex Hilbert space \(\mathcal {H}\) . A symmetric operator T on \(\mathcal {H}\) is called a time operator of H if, for all \(t\in \mathbb {R}\) , \(e^{-itH}D(T)\subset D(T)\) (D(T) denotes the domain of T) and \(Te^{-itH}\psi=e^{-itH}(T+t)\psi, \ \forall t\in \mathbb {R}, \forall \psi \in D(T)\) . In this paper, spectral properties of T are investigated. The following results are obtained: (i) If H is bounded below, then σ(T), the spectrum of T, is either \(\mathbb {C}\) (the set of complex numbers) or \(\{z\in \mathbb {C}| Im z \geq 0\}\) . (ii) If H is bounded above, then \(\sigma(T)\) is either \(\mathbb {C}\) or \(\{z\in \mathbb {C}| Im z \leq 0\}\) . (iii) If H is bounded, then \(\sigma(T)=\mathbb {C}\) . The spectrum of time operators of free Hamiltonians for both nonrelativistic and relativistic particles is exactly identified. Moreover spectral analysis is made on a generalized time operator.
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This work is supported by the Grant-in-Aid No.17340032 for Scientific Research from the JSPS.
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Arai, A. Spectrum of Time Operators. Lett Math Phys 80, 211–221 (2007). https://doi.org/10.1007/s11005-007-0158-y
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DOI: https://doi.org/10.1007/s11005-007-0158-y