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Solutions to Quantum Mechanics Homework Set 1 for PHY 389K, Assignments of Health sciences

The solutions to problem 1 to problem 4 of the homework set for the quantum mechanics course (phy 389k) at the university of texas at austin. The solutions cover topics such as the eigenvectors and eigenvalues of an operator, hermiticity, and the commutator of operators.

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Uploaded on 08/26/2009

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Download Solutions to Quantum Mechanics Homework Set 1 for PHY 389K and more Assignments Health sciences in PDF only on Docsity! PHY 389K Quantum Mechanics, Homework Set 1 Solutions Matthias Ihl 02/01/2008 Note: I will post updated versions of the homework solutions on my home- page: http://zippy.ph.utexas.edu/~msihl/teaching.html 1 Problem 1 We know that A|ai〉 = ai|ai〉. Therefore, f(A)|ai〉 = (A− a1)...(A− aN )(A− ai)|ai〉 = 0, (1) since one can commute the corresponding factor to the right. For an arbitrary state |ψ〉 = ∑N j=1 cj|aj〉, it follows that f(A)|ψ〉 = ∑ j cjf(A)|aj〉 = 0. (2) Since this is true for all |ψ〉, f(A) = 0 on the space spanned by {|ai〉}i. 2 Problem 2 (a) Hermiticity: (A†A)† = A†(A†)† = A†A. (3) (b) trace of A†A: Let U be a unitary transformation such that |bi〉 = Uij|aj〉, ∀i, j = 1, . . . , N. (4) 1 which rotates an arbitrary basis {|bi〉}i to the eigenbasis {|ai〉}i of A. Then, trA†A = trU †A†AU = ∑ i 〈ai|U †A†AU |ai〉 = ∑ i,j 〈ai|U †A†|bj〉〈bj|AU |ai〉 = ∑ i,j ∣ ∣ ∣ 〈bj |AU |ai〉 ∣ ∣ ∣ 2 = ∑ i,j ∣ ∣ ∣ 〈bj |A|bj〉 ∣ ∣ ∣ 2 . (c) Similarly, for 〈A†A〉, we get 〈ψ|A†A|ψ〉 = ∑ i,j 〈ai|c ∗ iA †Acj|aj〉 = ∑ i |ci| 2|ai| 2 ≥ 0. 3 Problem 3 We consider the operator ~S · ~n (see Sakurai, page 62). The fact that the unit vector ~n lies in the yz-plane means α = ±π. Moreover, β = γ in this problem. We will define |γ,+〉 := |~S · ~n,+;α = π, β = γ〉 = cos γ 2 |+〉 + i sin γ 2 |−〉. (5) The probability that anmSz = − ~ 2 atom is accepted by the second experiment is given by: P2 = |〈γ,+|−〉| 2 = sin2 γ 2 . (6) Likewise, for the third experiment, we get P3 = |〈−|γ,+〉| 2 = sin2 γ 2 . (7) This is maximized for γ = π.
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