Complementarity (physics)
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In physics, complementarity is a basic principle of quantum theory, and refers to effects
such as the wave-particle duality, in which different measurements made on a system reveal
it to have either particle-like or wave-like properties. Niels Bohr is usually associated
with this concept; in the orthodox form, it is stated that a quantum mechanical system
consisting of a boson or fermion can either behave as a particle or as wave, but never
simultaneously as both. A less orthodox interpretation is the "duality condition,"
described by the inequality due to Englert (see Phys. Rev. Lett., Vol. 77, 2154 (1996)),
which allows wave and particle attributes to co-exist, but postulates that a stronger
manifestation of the particle nature leads to a weaker manifestation of the wave nature
and vice versa.
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The emergence of complementarity in a system occurs when one considers the circumstances
under which one attempts to measure its properties; as Bohr noted, the principle of
complementarity "implies the impossibility of any sharp separation between the behaviour
of atomic objects and the interaction with the measuring instruments which serve to define
the conditions under which the phenomena appear." It is important to distinguish, as did
Bohr in his original statements, the principle of complementarity from a statement of the
uncertainty principle. For a technical discussion of contemporary issues surrounding
complementarity in physics, see, e.g., [1] (from which parts of this discussion were
drawn.)
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Various neutron interferometry experiments demonstrate the subtleness of the notions of
duality and complementarity in an interesting way. In order to pass through the
interferometer, the neutron must act as a wave. Yet upon passage, the neutron is subject
to gravitation, which one would think only particles, and not waves, are subject to. As
the neutron interferometer is rotated through Earth's gravitational field a phase change
between the two arms of the interferometer is created, resulting in a change in the
constructive and destructive interference of the neutron waves on exit from the
interferometer. Note that in order to understand the interference effect one must concede
that a single neutron takes both paths through the interferometer at the same time: a
single neutron must "be in two places at once", as it were. Since the two paths through a
neutron interferometer can be as far as five to 15 cm apart, the effect is hardly
microscopic. This is in contrast to traditional double-slit experiments where the slits
are less than one mm apart. Adding to the intellectual drama is that the neutron is a
baryon, a rather massive, slow-moving fermion, and thus not ephemeral in the way that a
photon (a boson) is.
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The Afshar experiment is claimed to question the validity of the principle of
complementarity in quantum mechanics. However, see rebuttals by Unruh [2] and Kastner [3].
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