PHYS 455 Short Answers to Homework III
PHYS 455 Short Answers to Homework III PHYS 455 Short Answers to Homework III
As a result, the results obtained and the final collapsed state does not depend on theorder which the individual measurements are carried out. The same conclusion willalso be true between the local measurements described here and a single measurementof these three observables when these three particles are together.However, the intermediate collapsed states will depend on the order as the exampleabove illustrates. Moreover, the possibilities of different results at the time of theexperiment depends on the order (for this example, the last person doing the measurementgets a definite result depending on the results of previous two measurements).This is why the Cophenagen interpretation is problemmatic for relativity. If Alice,Bob and Charlie are at very distant locations in space and they do their measurementsat more or less same times, then there will be different reference frames (moving withdifferent velocities) such that observers in these frames will see different orders forthese measurements. As a result, different observers will describe the intermediatecollapsed states differently, even though they are describing the same physical events.(However, the final collapsed state, results and their probabilities will be the same forevery observer.)2. (a) Using the matrix representation we haveρ = ∑ p α ψ α ψ α † = 1 [ ] 1 0+ 1 [ ]1 1 1+ 1 13 0 0 3 2 1 1 3 2α[ 1 −ii 1]= 1 [64 1 − i1 + i 2].(b) LetQ + =[ 1 00 0]Q − =[ 0 00 1be the respective projectors onto the spin-up and spin-down states along z axis.ThenP + = tr Q + ρ = tr 1 [ ] 4 0= 2 ,6 0 0 3and similarly for P − = tr Q − ρ = 1/3. These probabilities can be equivalentlycomputed asP + = 〈↑ |ρ| ↑〉 = 2 3]P − = 〈↓ |ρ| ↓〉 = 1 3(c) 〈σ x 〉 = tr σ x ρ = 1/3, etc. We get 〈σ y 〉 = 〈σ z 〉 = 1/3 also. In other words,,.〈⃗σ〉 = ˆx + ŷ + ẑ3.3. (a,b) Show.(c) We find tr ⃗σ · ⃗u = 0 and tr (⃗σ · ⃗u)(⃗σ · ⃗v) = 2⃗u · ⃗v.2
4. ρ is a density matrix for a spin 1/2 particle for which 〈⃗σ〉 = ⃗a.5. (a)(a) 〈σ n 〉 = 〈⃗σ〉 · ˆn = ⃗a · ˆn.(b) Basically we should have −1 ≤ ⃗a · ˆn ≤ 1 for any unit vector ˆn. This shows thatthe length of ⃗a is at most 1. To show this more elegantly, we choose ˆn = ⃗a/ |⃗a|,i.e., unit vector parallel to ⃗a. In that case, we have ⃗a · ˆn = |⃗a|. The inequalitythen says that |⃗a| ≤ 1.(c) The general expression for a hermitian 2×2 matrix: ρ = c 0 I +c 1 σ x +c 2 σ y +c 3 σ z =c 0 I +⃗c ·⃗σ. Now, using what is known about ρ we get tr ρ = 2c 0 = 1 and thereforec 0 = 1/2. Also, a x = 〈σ x 〉 = tr σ x ρ = 2c 1 etc. gives ⃗c = ⃗a/2. This is the finalexpression for ρI + ⃗a · ⃗σρ = .2In other words, in this two-dimensional space a density matrix ρ is completelydetermined by 〈⃗σ〉, the expectation values of the three Pauli spin matrices. (Tomeasure the density matrix of an ensemble, we just need to measure the averageof these three observables.)(e) Let ˆn = ⃗a/ |⃗a|, i.e., same unit vector used in part (b). In that case, ⃗a · ⃗σ = |⃗a| σ nandρ = I + |⃗a| σ n.2Therefore, the eigenvectors of ρ are |ˆn ↑〉 and |ˆn ↓〉. The corresponding eigenvaluesare then (1 ± |⃗a|)/2.(f) The density matrix is positive semidefinite means that all of its eigenvalues arenon-negative. This is equivalent to |⃗a| ≤ 1 in this case.(g) ρ represents a pure state if ρ has a single eigenvalue equal to 1 and the rest of itseigenvalues are 0. This can happen if and only if |⃗a| = 1.ρ A = tr BC |GHZ〉 〈GHZ|1= tr BC (|↑↑↑〉 〈↑↑↑| + |↑↑↑〉 〈↓↓↓| + |↓↓↓〉 〈↑↑↑| + |↓↓↓〉 〈↓↓↓|)21= tr BC (|↑〉 〈↑| ⊗ |↑↑〉 〈↑↑| + |↑〉 〈↓| ⊗ |↑↑〉 〈↓↓|2+ |↓〉 〈↑| ⊗ |↓↓〉 〈↑↑| + |↓〉 〈↓| ⊗ |↓↓〉 〈↓↓|)= 1 (|↑〉 〈↑| 〈↑↑ | ↑↑〉 + |↑〉 〈↓| 〈↓↓ | ↑↑〉2+ |↓〉 〈↑| 〈↑↑ | ↓↓〉 + |↓〉 〈↓| 〈↓↓ | ↓↓〉)= 1 2 (|↑〉 〈↑| + |↓〉 〈↓|) = 1 2 I AAs the |GHZ〉 state is very symmetric among the three particles, the same resultsare obtained for the other two parties, i.e., ρ B = I B /2 and ρ C = I C /2. Here, I Ais the identity operator for Alice’s particle etc.3
As a result, the results obtained and the final collapsed state does not depend on theorder which the individual measurements are carried out. The same conclusion willalso be true between the local measurements described here and a single measuremen<strong>to</strong>f these three observables when these three particles are <strong>to</strong>gether.However, the intermediate collapsed states will depend on the order as the exampleabove illustrates. Moreover, the possibilities of different results at the time of theexperiment depends on the order (for this example, the last person doing the measurementgets a definite result depending on the results of previous two measurements).This is why the Cophenagen interpretation is problemmatic for relativity. If Alice,Bob and Charlie are at very distant locations in space and they do their measurementsat more or less same times, then there will be different reference frames (moving withdifferent velocities) such that observers in these frames will see different orders forthese measurements. As a result, different observers will describe the intermediatecollapsed states differently, even though they are describing the same physical events.(However, the final collapsed state, results and their probabilities will be the same forevery observer.)2. (a) Using the matrix representation we haveρ = ∑ p α ψ α ψ α † = 1 [ ] 1 0+ 1 [ ]1 1 1+ 1 13 0 0 3 2 1 1 3 2α[ 1 −ii 1]= 1 [64 1 − i1 + i 2].(b) LetQ + =[ 1 00 0]Q − =[ 0 00 1be the respective projec<strong>to</strong>rs on<strong>to</strong> the spin-up and spin-down states along z axis.ThenP + = tr Q + ρ = tr 1 [ ] 4 0= 2 ,6 0 0 3and similarly for P − = tr Q − ρ = 1/3. These probabilities can be equivalentlycomputed asP + = 〈↑ |ρ| ↑〉 = 2 3]P − = 〈↓ |ρ| ↓〉 = 1 3(c) 〈σ x 〉 = tr σ x ρ = 1/3, etc. We get 〈σ y 〉 = 〈σ z 〉 = 1/3 also. In other words,,.〈⃗σ〉 = ˆx + ŷ + ẑ3.3. (a,b) Show.(c) We find tr ⃗σ · ⃗u = 0 and tr (⃗σ · ⃗u)(⃗σ · ⃗v) = 2⃗u · ⃗v.2
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