Here's another experiment that is extremely
straightforward and simple.

We know that thermo noise has no theoretical upper
crest limit. Normally we refer to noise in terms of
root mean square. When studying real thermo noise we
see that given enough time the noise will eventually
drift to a higher crest. The experiment is simple.
Connect one resistor in series with an LED. That is
it. To save yourself a lot of time you should pick a
high frequency LED as used in GHz optics. This will
provide a lot of bandwidth, which is what you want
given voltage thermo noise is (4 K T R B)^0.5, where B
= Bandwidth.  Also you want to pick a resistor that
matches the LED for an optimum effect. Also it doesn't
hurt if the resistor is a noisy one such as carbon
composite and as small as possible. Smaller carbon
composite resistors generate more noise. Of course the
*extra* noise is 1/f. This results in a resistor with
real noise. When then voltage noise crest overcomes
the LED's forward voltage then the LED will emit
photon(s).  Also note the LED emits photons far below
the forward voltage. So in that sense, it is possible
the LED will emit an occasional photon even when the
noise voltage is far below the LED's forward voltage.

Now the question is, "Where do we aim the photons?" 
Note the above experiment is in an isolated system. We
have two experiments. Experiment #1, the resistor
absorbs the photons.  Experiment #2, the LED absorbs
its own photons (we coat the LED with opaque
material).  The main difference between the two
experiments is the resistor in experiment #2 is colder
than the resistor in experiment #1.


Note, the above experiments could require vast amounts
of time, depending on the exact parts used in such
experiments. Given enough time, the noise crest will
reach the LED's forward voltage. For those who are
less patient, it is possible you will see some photons
emitted even below the LED's forward voltage.

Regards,
Paul Lowrance



 
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