Let Y(r, t) = 4(r)etot be the wavefunction of a free particle of mass m, harmonically oscillating in time. Putting W(r, t) into the Schrödinger equation and eliminating the exponentials, we obtain -V²µ = Eµ, 2m where E = wh. Since, in general, only certain quantized values of the energy E are allowable, this equation can be interpreted as an eigenvalue problem for the Laplacian operator. Find the eigenstates y and corresponding energy levels E for a free particle, enclosed in a rectangular box with edge lengths a, b, and c. Assume that the wave function vanishes at the box faces.
Let Y(r, t) = 4(r)etot be the wavefunction of a free particle of mass m, harmonically oscillating in time. Putting W(r, t) into the Schrödinger equation and eliminating the exponentials, we obtain -V²µ = Eµ, 2m where E = wh. Since, in general, only certain quantized values of the energy E are allowable, this equation can be interpreted as an eigenvalue problem for the Laplacian operator. Find the eigenstates y and corresponding energy levels E for a free particle, enclosed in a rectangular box with edge lengths a, b, and c. Assume that the wave function vanishes at the box faces.
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