Characteristic time operators as quantum clocks

TL;DR

This paper explores a bounded, self-adjoint characteristic time operator that acts as a quantum clock near specific times, satisfying the canonical relation with the Hamiltonian and saturating the time-energy uncertainty relation.

Contribution

It demonstrates that the characteristic time operator can serve as a quantum clock in a neighborhood of certain times, despite not being covariant, by satisfying the canonical relation on a measure-zero set.

Findings

The operator satisfies the canonical relation on a measure-zero set of times.

Near these times, the operator's expectation value provides the parametric time.

The two-dimensional projection of the operator saturates the time-energy uncertainty relation.

Abstract

We consider the characteristic time operator $\mathsf{T}$ introduced in [E. A. Galapon, Proc. R. Soc. Lond. A, 458:2671 (2002)] which is bounded and self-adjoint. For a semibounded discrete Hamiltonian $\mathsf{H}$ with some growth condition, $\mathsf{T}$ satisfies the canonical relation $[\mathsf{T},\mathsf{H}]|\psi\rangle=i\hbar|\psi\rangle$ for $|\psi\rangle$ in a dense subspace of the Hilbert space. While $\mathsf{T}$ is not covariant, we show that it still satisfies the canonical relation in a set of times of total measure zero called the time invariant set $\mathscr{T}$. In the neighborhood of each time $t$ in $\mathscr{T}$, $\mathsf{T}$ is still canonically conjugate to $\mathsf{H}$ and its expectation value gives the parametric time. Its two-dimensional projection saturates the time-energy uncertainty relation in the neighborhood of $\mathscr{T}$, and is proportional to the Pauli matrix $\sigma_y$. Thus, one can construct a quantum clock that tells the time in the neighborhood of $\mathscr{T}$ by measuring a compatible observable.