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\(\S 13.2\) Particle in a Box and Square Well

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Three methods

  •        $\delta$ function potential as limit of square well
  •        Direct integration of the Schrodinger equation 
  •        Solution in Momentum Space

 are used to solve for the bound state energy eignevalue of the Dirac delta function  potential  \( V(x) = - g\delta(x) \).

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