Stern–Gerlach Sequential Measurements
Follow spin measurement branches and distinguish forgetting outcomes from postselection.
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Stern–Gerlach Sequential Measurements
Follow spin measurement branches and distinguish forgetting outcomes from postselection.
Worked Example
Consider an initial spin-1/2 system in state |+z>. An intermediate measurement is performed along an axis n lying in the xz plane at angle θ from +z, followed by a final measurement along +z. Let θ = 90° and the operation be "Measure and forget".
- Initial state: |ψ0> = |+z>
- Intermediate axis n: θ = 90°
- Intermediate + probability: |<+n|+z>|2 = cos2(θ/2) = cos2(45°) = 0.5
- Intermediate - probability: |<-n|+z>|2 = sin2(θ/2) = sin2(45°) = 0.5
- Measure and forget implies a nonselective measurement. The final density matrix is a mixed state.
- Final + probability given intermediate +: |<+z|+n>|2 = cos2(45°) = 0.5
- Final + probability given intermediate -: |<+z|-n>|2 = sin2(45°) = 0.5
- Final conditional + probability: 0.5 * 0.5 + 0.5 * 0.5 = 0.5
In this scenario, we obtain a final conditional +z probability of 0.5. Since we retain all branches (nonselective), the retained fraction is 1, and the joint retained and final + is also 0.5.
Experiment
Open the Stern–Gerlach Sequential Measurements module to interact with the apparatus.
- Set the Intermediate axis degrees to 90°.
- Set the Intermediate operation to Keep plus only.
- Observe the intermediate + probability becomes 0.5, and the retained fraction drops to 0.5, because we discard the |−n> branch.
- The final + conditional probability is 0.5, leaving a joint retained and final + probability of 0.25.
- Compare this with setting the operation to No measurement, where the state remains undisturbed |+z> and the final + conditional probability is 1.
Limitations
The diagram does not represent magnetic precession evolution; this module isolates the effect of measurement back-action. It assumes ideal, instantaneous measurements described by projection operators, ignoring continuous measurement dynamics and non-ideal detector efficiencies.
References
For a detailed theoretical treatment of Stern-Gerlach experiments and sequential measurements, see:
Experience it interactively
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