Physical Significance of G. Application to the Free Particle Case
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The general theory developed in Chap.l 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 presentend in Chap.2 is applicable to the time dependent one particle Schrödinger equation.
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