Momentum eigenfunctions proof and Fourier Transform question
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The discussion centers on defining the operator ##\Psi## and its eigenfunctions in quantum mechanics. Participants clarify that the eigenfunctions of the momentum operator in position representation and the position operator in momentum representation are not related through Fourier transformation, despite both representing the same state in different spaces. The presence of subscripts in the functions ##\psi_{\mathbf{k}}(\mathbf{r})## and ##\phi_{\mathbf{r}}(\mathbf{k})## indicates they correspond to different states and operators. Additionally, the sign difference in the exponents of these functions is explained in relation to the momentum operator's definition. Understanding these distinctions is crucial for grasping the fundamentals of quantum mechanics.
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