Abstract
We show that the dynamics for a particle confined in one-dimensional infinite square well with a mobile boundary can be converted to the case as if the boundary is time-independent at the expense of an appropriate time-dependent Hamiltonian. The Hamiltonian is deduced by the technique of integration within an ordered product of operators.
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Fan, Hy., Wu, H. Squeezing Dynamics for One-Dimensional Infinite Square Well with a Mobile Wall. Int J Theor Phys 48, 637–641 (2009). https://doi.org/10.1007/s10773-008-9830-y
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DOI: https://doi.org/10.1007/s10773-008-9830-y