Problem 1, solution
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Problem 2, solution|11>=|++>, From symmetry we therefore have that the common eigenfunctions of S2 and Sx are |11>x=|++>x, We have |++>x=(1/2)1/2(|+>+|->)Ä(1/2)1/2(|+>+|->)=(1/2)(|++>+|+->+|-+>+|-->). Therefore |11>x=(1/2)(|++>+|+->+|-+>+|-->), | |
Problem
3, solution
(a) The eigenvectors of Sy are |+>y=2-1/2(|+>+i|->) and |->y=2-1/2(|+>-i|->). Therefore: |+>=2-1/2(|+>y+|->y) and |->=(-i/21/2)(|+>y-|->y). |y1>=|+>y. |y2>=(-i/61/2)(|+>y+|->y) -(i/31/2)(|+>y-|->y)=(-i)(0.986|+>y+0.169|->y (b) <y1|y2>=-i/61/2-i(2/6)1/2=-i0.986 in the Sz basis. <y1|y2>=-i0.986 in the Sy basis. (c) |y1(t)>=2-1/2(exp(-iw0t/2)|+>+iexp(iw0t/2)|->)
=(h/4)i(-exp(-iw0t)+exp(iw0t))= -(h/2)sin(w0t). If <Sx>=±(h/2), then |y1(t)> is an eigenvector of Sx. This happens when w0t=np/2, n=odd. Problem
4, solution
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