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this paper explicitly reconstructs the derivation of the time-dependent Schr¨odinger equationfrom Richard Feynman’s path integral formulation (1948). By rigorously applying the scalecut-off condition (η ∼ √ϵ) and evaluating the Gaussian probability amplitudes term by term,we demonstrate the bottom-up emergence of the Hamiltonian operator without relying ona priori top-down classical assumptions.
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pureaum Jeon (2026) studied this question.
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