Fluctuations in the flow of electrons signal the transition
from particle to wave behavior. Published in
revised form in Physics Today, May 2003, page 37.
Carlo Beenakker & Christian Sch¨onenberger
“The noise is the signal” was a saying of Rolf Landauer,
one of the founding fathers of mesoscopic physics. What
he meant is that fluctuations in time of a measurement
can be a source of information that is not present in the
time-averaged value. A physicist may delight in noise, in
a way reminiscent of figure 1.
Noise plays a uniquely informative role in connection
with the particle-wave duality. It was Albert Einstein
who first realized (in 1909) that electromagnetic fluctuations
are different if the energy is carried by waves or
by particles. The magnitude of energy fluctuations scales
linearly with the mean energy for classical waves, but it
scales with the square root of the mean energy for classical
particles. Since a photon is neither a classical wave
nor a classical particle, the linear and square-root contributions
coexist. Typically, the square-root (particle)
contribution dominates at optical frequencies, while the
linear (wave) contribution takes over at radio frequencies.
If Newton could have measured noise, he would
have been able to settle his dispute with Huygens on the
corpuscular nature of light — without actually needing
to observe an individual photon. Such is the power of
noise.
The diagnostic property of photon noise was further
developed in the 1960’s, when it was discovered that
fluctuations can tell the difference between the radiation
from a laser and from a black body: For a laser the wave
contribution to the fluctuations is entirely absent, while
it is merely small for a black body. Noise measurements
are now a routine technique in quantum optics and the
quantum mechanical theory of photon statistics (due to
Roy Glauber) is textbook material.
Since electrons share the particle-wave duality with
photons, one might expect fluctuations in the electrical
current to play a similar diagnostic role. Current fluctuations
due to the discreteness of the electrical charge are
known as “shot noise”. Although the first observations
of shot noise date from work in the 1920’s on vacuum
tubes, our quantum mechanical understanding of electronic
shot noise has progressed more slowly than for
photons. Much of the physical information it contains
has been appreciated only recently, from experiments on
nanoscale conductors.1