Chapter 4: Q28P (page 177)
For the most general normalized spinor (Equation 4.139),
compute
Short Answer
By solving we find the above value to be.
Chapter 4: Q28P (page 177)
For the most general normalized spinor (Equation 4.139),
compute
By solving we find the above value to be.
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Get started for freeConsider the three-dimensional harmonic oscillator, for which the potential is
(a) Show that separation of variables in cartesian coordinates turns this into three one-dimensional oscillators, and exploit your knowledge of the latter to determine the allowed energies. Answer:
(b) Determine the degeneracyof
In Problem4.3 you showed that . Apply the raising operator to find localid="1656065252558" . Use Equation 4.121to get the normalization.
Use equations 4.27 4.28 and 4.32 to construct Check that they are normalized and orthogonal
Determine the commutator of with(where) Generalize your result to show that
Comment: Because does not commute with , we cannot hope to find states that are simultaneous eigenvectors of both. In order to form eigenstates ofweneed linear combinations of eigenstates of. This is precisely what the Clebsch-Gordan coefficients (in Equation 4.185) do for us, On the other hand, it follows by obvious inference from Equation 4.187that the sumrole="math" localid="1655980965321" does commute withdata-custom-editor="chemistry" , which is a special case of something we already knew (see Equation 4.103).
Use separation of variables in Cartesian coordinates to solve infinite cubical well
if x,y,z are all between 0 to a;
Otherwise
a) Find the stationary states and the corresponding energies
b) Call the distinct energies in the order of increasing energy. Findlocalid="1658127758806" determine their degeneracies (that is, the number of different states that share the same energy). Comment: In one dimension degenerate bound states do not occur but in three dimensions they are very common.
c) What is the degeneracy of E14 and why is this case interesting?
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