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Realy ascrqu ment ; Sects Vit y id (2
P 167), Sect. 2.3 (ap 18 p. 172).
1. The deuteron ig a physical system composed of a proton with angular momentum j, = Jproton = 4 and
a neutron with angular momentum j= jrewron = ¥4.
a) Considering only rotational degrees of freedom, what is the space of physical states of the
deuteron?
b) Give the explicit expressions for the eigenvectors of deuteron angular momentum J in terms of
the product basis vectors of jproton ANG freuwon-
¢) Calculate the expectation value of the operator J” - J’ pon - Fnewron for all the deuteron states.
- Consider the combination of two rotators with * = 4 and j= 4. Start with the direct product basis
vectors [J" m") @ LP m®) = |'4, 4) @ |'4, ys |94, 4) @ [4, “14s [4) @ [4 A): |4, 14 @ IA, 4).
a)
b)
e)
d)
Gy
4,
Which of these vectors are eigenvectors of J? = (J + 9
Form linear combinations of the remaining direct product vectors which are not eigenvectors of
J to obtain normalized eigenvectors of J’. Check whether these are orthogonal to each other
and to the vectors found in a.
Calculate the action of Jz = J iJ, on the eigenvectors of F.
Compare the coefficients that you found in b) with C G coefficients (44 m* ‘4m? | % 14 7 m) in
Table 2.1, Sect. V.2 of the textbook.
To evaluate the usefulness of the Wigner-Eckart theorem compare the number of
matrix elements (j'm'|V2""|j m) with the number of reduced matrix elements (7" |]
V? || 7) for a vector V.
Show that the reduced matrix element for the angular momentum operator J, is given
by
GU FM} = 8590 +1)
when the reduced matrix element is normalized as in (3.6). Compare this normaliza-
tion with the normalization in your other favorite quantum mechanics books.