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1 Lecture 3: The many body problem 2 The Schrödinger equation
1 Lecture 3: The many body problem 2 The Schrödinger equation

... wavefunctions. For example, ψjk (xk ) could be the eigenfunctions of the harmonic oscillator. Then any product ψj1 (x1 )ψj2 (x2 ) · · · ψjN (xN ) is a valid many-body wavefunction. Further, these products are complete, in that any many-body wavefunction can be expressed as a linear combination of th ...
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Bra–ket notation

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