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Next: 4.3 Quantum Ontologies
Up: 4. The Peculiarities of
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4.2 Quantum Experiments
It is not the place here to describe in detail all the experiments that
manifest the peculiar phenomena of quantum physics, so I will have to
assume some previous acquaintance with the quantum problems.
There are a great many semi-popular introductory books (e.g. Herbert
[1985] or Rae [1986]) which describe the basic experiments demonstrating
quantum peculiarities. I presume some acquaintance with this material, so
here I need merely point out the existence of experiments such as:
- The photo-electric effect, where light interacts with electrons in
discrete units called quanta as if it was made of particles.
These particles (the quanta of the light field) are called photons.
- The two-slit interference experiment, where both light, electrons,
and neutrons (and even composite atoms) produce oscillatory interference
effects as if they were waves.
- Interferometer experiments (see e.g. Zeilinger [1986]) which verify
the wave nature of light and neutrons to high accuracy. Both light and
neutrons beams are here split up into several components that are observed
to remain coherent with each other even after several reflections from
mirrors. The mirrors of course are composed of many atoms -- the
beams are reflected coherently from all these atoms.
- Einstein-Podolsky-Rosen (EPR) types of experiments4.1, where two particles emitted in single event retain a correlation as
if they were continually connected even when a long way apart. These
non-local correlations have been quantified in terms of Bell's
Inequalities (Bell [1964]), and have been experimentally verified in a
large number of experiments (see Clauser & Shimony [1978]). Aspect et al.
[1982] have observed these non-local connections persisting even when
any communication between the particles would have to travel faster than
light.
- `Quantum Beat' experiments (see Andrä [1970]), where a
hydrogen atom is excited into a superposition of two excited states, and
oscillatory beats are observed when the two states decay together
coherently.
- Tunnelling phenomena, such as the slow decay rate of radioactive
nuclei. Here, a particle (or cluster of particles) is confined to move
inside the nucleus by nuclear potentials that stop it from getting too
far from the centre. However, it can slowly `leak out' by tunnelling
through the potential barrier.
- Aharanov-Bohm effect (Aharanov & Bohm [1959]), where an electron beam
is passed around both sides of a long thin solenoid containing a magnetic
field. Although the magnetic field can be completely confined within the
solenoid, there are observed interference oscillations between the parts
of the beam that pass on the two sides. These oscillations depend on the
strength of the magnetic field, even though the electrons never enter a
region of space where the magnetic field is non-zero.
- Scattering experiments between (say) two electrons show oscillatory
fluctuations in the scattering rate that can only be explained if the two
electrons are strictly indistinguishable.
Next: 4.3 Quantum Ontologies
Up: 4. The Peculiarities of
Previous: 4.1 Classical and Quantum
Prof Ian Thompson
2003-02-25
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