Quantum Mechanics 101 · Unit 3: The Mathematical Machinery
Quantum Academy · Chapter 15: Superposition & Measurement
Both, neither, and the moment the dice are thrown
Part A Vocabulary matching
Write the letter of the matching definition in the blank beside each term.
- 1.Superposition
- 2.Probability amplitude
- 3.Normalization
- 4.Basis
- 5.Relative phase
- 6.Mixture
- 7.Projective measurement
- 8.Collapse
- 9.Incompatible observables
- 10.Quantum Zeno effect
- 11.Measurement problem
- 12.Decoherence
- A.The projection postulate: the update of the state to the eigenstate matching a measurement result; whether it is a physical process is interpretation-dependent.
- B.A complete set of perfectly distinguishable states, such as |0⟩ and |1⟩ or |+⟩ and |−⟩, in terms of which any state can be written.
- C.A probabilistic blend of definite states that reflects ignorance, like a coin under a cup; unlike a superposition, it produces no interference.
- D.The loss of observable interference when a system becomes entangled with its environment, which records information about it.
- E.A state written as a weighted sum of other states, such as α|0⟩ + β|1⟩; a single definite state whose outcomes are uncertain only for measurements in a basis that does not contain it.
- F.The conflict between linear, unitary evolution, which predicts superpositions of pointer readings, and the single definite outcomes every experiment records.
- G.Observables whose operators do not commute, such as Z and X, so that no state has definite values of both and measuring one randomizes the other.
- H.A complex coefficient in a superposition; the squared magnitude of an amplitude gives the probability of the matching outcome.
- I.The suppression of a quantum transition by frequent measurements, which repeatedly return the system to its initial state.
- J.An ideal measurement whose results are the eigenvalues of an observable, with probabilities given by the Born rule, leaving the system in the matching eigenstate.
- K.The phase difference between the amplitudes in a superposition; invisible to some measurements but decisive for interference.
- L.The requirement that the squared magnitudes of all amplitudes add to one, so that the outcome probabilities sum to 1.
Part B Questions
- 1.
Which of these is a properly normalized qubit state?Circle one
- A0.5|0⟩ + 0.5|1⟩
- B0.8|0⟩ + 0.8|1⟩
- C0.6|0⟩ − 0.8i|1⟩
- D|0⟩ + |1⟩
- 2.
Box P holds qubits in the state |+⟩; box Q holds qubits secretly set to |0⟩ or |1⟩ with even odds. Which single type of measurement, repeated on many qubits from each box, tells you which box is which?Circle one
- AZ measurements, because the superposition gives 0 more often
- BX measurements, because only the superposition gives plus every time
- CTwo Z measurements in a row on each qubit, to see whether the answer changes
- DNone, because the two boxes are physically identical
- 3.
A qubit is measured in Z and gives 0. It is then measured in X and gives minus. What is the probability that a third measurement, in Z, gives 0?Circle one
- A0
- B0.25
- C0.5
- D1
- 4.
Two qubit states with the same values of |α|² and |β|² give the same statistics for every possible measurement.Circle one
TrueFalse
- 5.
An ideal projective Z measurement repeated immediately on the same qubit can give 0 the first time and 1 the second.Circle one
TrueFalse
- 6.
Decoherence explains why interference between macroscopically different states becomes unobservable, but by itself it does not select which single outcome occurs.Circle one
TrueFalse
- 7.
A probabilistic blend of definite states, whose probabilities reflect only our ignorance, is called a .Fill in the blank
- 8.
The rule that leaves a system in the eigenstate matching the measured result is called the projection postulate, or .Fill in the blank
- 9.
State the measurement problem in your own words. Your answer should mention linearity.Short answer
- 10.
A friend says the quantum Zeno effect proves that a conscious observer controls reality. Use the NIST experiment to answer them.Short answer
- 11.
A qubit is prepared in |ψ⟩ = (1/√3)|0⟩ + √(2/3)|1⟩. Show that it is normalized, find the probability of each Z result, and predict the number of 1 results in 600 runs, with the binomial standard deviation √(N·p·(1 − p)).Show your working
WorkingAnswer:
- 12.
A qubit is prepared with θ = 90° and φ = 60°. Find the probability of 0 in a Z measurement and of plus in an X measurement. What would a fifty-fifty mixture of |0⟩ and |1⟩ give in X?Show your working
WorkingAnswer:
- 13.
A drive would rotate a qubit fully from |0⟩ to |1⟩ in a time T, and you make N equally spaced Z measurements during it. (a) Find the probability the qubit is found in |0⟩ at every check for N = 20. (b) Use the approximation 1 − π²/(4N) to estimate how many checks keep the survival probability at 99 percent or more, then check your estimate with the exact formula.Show your working
WorkingAnswer:
- 14.
An 8.0 mW unpolarized beam passes four polarizers in a row, with axes at 0°, 30°, 60° and 90°. What power emerges? Compare with two crossed polarizers at 0° and 90° alone.Show your working
WorkingAnswer:
Part C Mad scientist challenge bonus
The measurement problem meets decoherence. A qubit starts in α|0⟩ + β|1⟩ with real amplitudes, and a detector records it, so that the combined state becomes α|0⟩|A₀⟩ + β|1⟩|A₁⟩, where the pointer states are normalized and have real overlap c = ⟨A₀|A₁⟩. (a) Rewrite the combined state using |0⟩ = (1/√2)(|+⟩ + |−⟩) and |1⟩ = (1/√2)(|+⟩ − |−⟩), and show that the probability of finding the qubit in |+⟩ is one half of (1 + 2αβc). (b) Evaluate it for α = β = 1/√2 when the detector records nothing (c = 1), records partially (c = 0.6), and records perfectly (c = 0). (c) Evaluate it for α = 0.6, β = 0.8 and c = 0.5. (d) Explain what this has to do with why a dust grain in air never shows interference.