Abstract
The Lewis and Riesenfeld method is used by Ramos et al. (Eur. Phys. J. Plus 133, 449 2018) to study quantum systems governed by time-dependent \(\mathcal {P}\mathcal {T}\) symmetric Hamiltonians and particularly where the quantum system is a particle submitted to the action of a complex time-dependent linear potential. They have misleadingly claim that the \(\mathcal {P}\mathcal {T}\) invariant eigenstates are normalized with the Dirac delta function and obtained non physical observable expectation values of the position and the momentum operators x and p, as a consequence there is no uncertainty product for this system. We discuss and correct their results using the pseudo-invariant approach. To this end, we introduce a linear pseudo hermitian invariant operator which allows us to solve analytically the time-dependent Schrödinger equation for this problem and to construct a Gaussian wave packet solution. The normalization condition for the invariant eigenfunctions with the Dirac delta function is obtained. Then, using this Gaussian wave packet, we calculate the expectation values of the position and the momentum as well as the uncertainty product. We find that these expectation values of x and p are complex numbers but describe the classical motion. Also, we show that the uncertainty relation is physically acceptable.
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Notes
The authors of Ref. [1] wrote (29), this means that eigenstates ϕλ(x,t) of the invariant operator I(t) are transformed under the \(\mathcal {P}\mathcal {T}\) action as \(\mathcal {P}\mathcal {T}{\phi }_{\lambda }(x,t)={\phi }_{\lambda }^{\ast }(-x,t).\) This implies that the eigenstates ϕλ(x,t) of I(t) are NOT eigenstates of the \(\mathcal {P}\mathcal {T}\) operator as claimed by the authors of Ref. [1]. One can see that in the following
$$ \begin{array}{@{}rcl@{}} PT\phi_{\lambda}(x,t) &=& \sqrt{\frac{\sigma_{\lambda}}{2\pi b^{\ast}(t)}}\exp\left\{ \frac{-i}{b^{\ast}(t)}\left[ \left( \lambda-\gamma^{\ast}(t)\right) (-x)-\frac{a_{0}^{\ast}}{2}x^{2}\right] \right\} \\ &=& \sqrt{\frac{\sigma_{\lambda}}{-2\pi b(t)}}\exp\left\{ \frac{-i} {b(t)}\left[ \left( \lambda-c(t)\right) x-\frac{a_{0}}{2}x^{2}\right] \right\} \text{ \ }\\ && \neq\phi_{\lambda}(x,t). \end{array} $$(27)Morever these eigenstates of I(t) will not also satisfy the normalization condition with the Dirac delta function
$$ {\int}_{-\infty}^{+\infty}\phi_{\lambda^{^{\prime}}}^{PT}(x,t)\phi_{\lambda }(x,t)dx=\frac{\sqrt{\sigma_{\lambda^{^{\prime}}}\sigma_{\lambda}}}{2\pi }\left[ \exp\frac{(\lambda-\lambda^{^{\prime}})}{\left\vert b(t)\right\vert }x\right]_{-\infty}^{+\infty} $$(28)where \(b(t)=i\left \vert b(t)\right \vert \) is purely imaginary.
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Koussa, W., Maamache, M. Pseudo-Invariant Approach for a Particle in a Complex Time-Dependent Linear Potential. Int J Theor Phys 59, 1490–1503 (2020). https://doi.org/10.1007/s10773-020-04417-0
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DOI: https://doi.org/10.1007/s10773-020-04417-0