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Re: [Phys-L] zero point motion and E-M emission



On 06/09/2013 10:25 PM, Bernard Cleyet wrote:

At zero there is energy available to emit radiation (E-M).

Hah! That's a good question. I remember asking myself
that question once upon a time. It took me a year to
figure out the answer.

Zero point motion is a fiction?

That's not the answer.

Consider a hydrogen atom in its ground state. The size
of the atom *is* the zero-point motion of the electron.
If there were no zero point motion, there would be no
atoms.

So, do you want the conventional answer or my answer?

*) The conventional answer is that the electron in
the ground state cannot radiate. If you do the math
using the usual energy-eigenstate photon-number
basis, you can more-or-less convince yourself that
this is true. Note that photon number is second
order in the ladder operators "a" and "a†".

*) However, we can also work things out in terms of
the /position/ of the electron and the /voltage/
of the electromagnetic field. This is a whole
different kettle of fish. Note that the voltage
is first order in the ladder operators "a" and "a†".

If you do the math this way, the electron does
radiate. It's an electron, and it's moving, so
how could it not radiate?

However, what's sauce for the goose is sauce for
the gander. There is also some zero-point excitation
in _every mode_ of the EM field ... and there are a
lot of modes. This electromagnetic radiation shines
on the electron and imparts energy to it.

If you do the math correctly, you find that the
energy going from the electron to the EM field
is exactly equal to the energy going the other
way, on average.


=========
This is true at any temperature, if the atom is
at the same temperature as the photon gas. Zero
temperature is just a special case ... and not
even very special. That is to say, the thermal
fluctuations do /not/ go to zero at T=0. Based
on extrapolation of the high-temperature behavior
you might have expected them to, but they don't.
The whole picture is diagrammed and explained here:
http://www.av8n.com/physics/oscillator.htm
=========

Hint: If you want to do this calculation yourself,
start with the one-dimensional field, i.e. the field
in a coaxial cable. The three-dimensional quantum
field theory is more work, but not significantly
more edificational.

Note that in the course of doing the calculation,
as a by-product, you will rederive the fluctuation-
dissipation theorem. Also, all of this is intimately
related to the second law of thermodynamics and to
the Heisenberg uncertainty principle.