Physical Significance of G. Application to the Free Particle Case
The general theory developed in Chap.1 can be applied directly to the time-independent one-particle Schrödinger equation by making the substitutions L(r) → H(r), λ → E, where H(r) is the Hamiltonian. The formalism presented in Chap.2 is applicable to the time-dependent one-particle Schrödinger equation.
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