Elitzur–Vaidman bomb tester

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Bomb-testing problem diagram. A - photon emitter, B - bomb to be tested, C,D - photon detectors. Mirrors in the lower left and upper right corners are half-silvered.
Quantum mechanics
Introduction
Glossary · History
Experiments

In physics, the Elitzur–Vaidman bomb-testing problem is a thought experiment in quantum mechanics, first proposed by Avshalom Elitzur and Lev Vaidman in 1993.[1] An actual experiment demonstrating the solution was constructed and successfully tested by Anton Zeilinger, Paul Kwiat, Harald Weinfurter, and Thomas Herzog from the University of Innsbruck, Austria and Mark A. Kasevich of Stanford University in 1994.[2] It employs a Mach–Zehnder interferometer for ascertaining whether a measurement has taken place.

Problem

Consider a collection of bombs, of which some, but not all, are duds. Suppose that these bombs possess certain properties: usable (non-dud) bombs have a photon-triggered sensor, which will absorb an incident photon and detonate the bomb. Dud bombs have a malfunctioning sensor, which will not interact with the photons in any way.[3] Thus, the dud bomb will not detect the photon and will not detonate. The problem is how to separate at least some of the usable bombs from the duds. A bomb sorter could accumulate dud bombs by attempting to detonate each one. Unfortunately, this naive process destroys all the usable bombs.

Solution

A solution is for the sorter to use a mode of observation known as counterfactual measurement, which relies on properties of quantum mechanics.[4]

Start with a Mach–Zehnder interferometer and a light source which emits single photons. When a photon emitted by the light source reaches a half-silvered plane mirror, it has equal chances of passing through or reflecting.[5] On one path, place a bomb (B) for the photon to encounter. If the bomb is working, then the photon is absorbed and triggers the bomb. If the bomb is non-functional, the photon will pass through the dud bomb unaffected.

When a photon's state is non-deterministically altered, such as interacting with a half-silvered mirror where it non-deterministically passes through or is reflected, the photon undergoes quantum superposition, whereby it takes on all possible states and can interact with itself. This phenomenon continues until an 'observer' (detector) interacts with it, causing the wave function to collapse and returning the photon to a deterministic state.

Step-by-step explanation

  • After being emitted, the photon 'probability wave' will both pass through the 1st half-silvered mirror (take the lower-route) and be reflected (take the upper-route).

If the bomb is a dud:

  • The bomb will not absorb a photon, and so the wave continues along the lower route to the second half silvered mirror (where it will encounter the upper wave and cause self-interference).
  • The system reduces to the basic Mach–Zehnder apparatus with no sample bomb, in which constructive interference occurs along the path horizontally exiting towards (D) and destructive interference occurs along the path vertically exiting towards (C).
  • Therefore, the detector at (D) will detect a photon, and the detector at (C) will not.

If the bomb is usable:

  • Upon meeting the observer (the bomb), the wave function collapses and the photon must be either on the lower route or on the upper route, but not both.
  • If the photon is measured on the lower route:
    • Because the bomb is usable, the photon is absorbed and triggers the bomb which explodes.
  • If the photon is measured on the upper route:
    • It will not encounter the bomb - but since the lower route can not have been taken, there will be no interference effect at the 2nd half-silvered mirror.
    • The photon on the upper route now both (i) passes through the 2nd half-silvered mirror and (ii) is reflected.
    • Upon meeting further observers (detector C and D), the wave function collapses again and the photon must be either at detector C or at detector D, but not both.

Thus we can state that if any photons are detected at (C), there must have been a working detector at (B) – the bomb position.

With this process, 25% of the usable bombs can be identified as usable without being consumed.[1] whilst 50% of the usable bombs will be consumed and 25% remain 'unknown'. By repeating the process with the 'unknowns', the ratio of surviving, identified, usable bombs approaches 33% of the initial population of usable bombs. See Experiments section below for a modified experiment that can identify the usable bombs with a yield rate approaching 100%.

This phenomenon may be seen as a form of weak coupling between worlds in the many-worlds interpretation.[citation needed]

Experiments

In 1994, Anton Zeilinger, Paul Kwiat, Harald Weinfurter, and Thomas Herzog actually performed an equivalent of the above experiment, proving interaction-free measurements are indeed possible.[2]

In 1996, Kwiat et al. devised a method, using a sequence of polarising devices, that efficiently increases the yield rate to a level arbitrarily close to one. The key idea is to split a fraction of the photon beam into a large number of beams of very small amplitude, and reflect all of them off the mirror, recombining them with the original beam afterwards.[6] ( See also http://www.nature.com/nature/journal/v439/n7079/full/nature04523.html#B1 .) It can also be argued that this revised construction is simply equivalent to a resonant cavity and the result looks much less shocking in this language. See Watanabe and Inoue (2000).

This experiment is philosophically significant because it determines the answer to a counterfactual question: "What would happen were the photon to go into the bomb sensor?". The answer is either: "the bomb would work, the photon would be observed, and the bomb would explode", or "the bomb is a dud, the photon would not be observed and it would pass through unimpeded". If we were to directly perform the measurement, any working bomb would actually explode. But here the answer to the question "what would happen" can be determined without a working bomb necessarily going off. This provides an example of an experimental method to answer a counterfactual question.

See also

References

  1. ↑ 1.0 1.1 Elitzur & Vaidman 1993
  2. ↑ 2.0 2.1 Experimental realization of "interaction-free" measurements, Paul Kwiat 1994
  3. ↑ Can Schrodinger's Cat Collapse the Wavefunction?, Keith Bowden 1997
  4. ↑ Keith Bowden (k.bowden@physics.bbk.ac.uk)
  5. ↑ David Harrison
  6. ↑ Tao of Interaction-Free Measurements, Paul Kwiat

Further reading

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