Fiziqs said:
As I mentioned in an earlier post I have a bit of a problem trying to see how the random scattering in denser mediums can provide "which path" information. How do you gain "which path" information from random scattering?
But because I lack an understanding of the intricacies of the experiments, I may well be missing something. If we set up a double slit experiment and we introduce progressively denser mediums, we would expect the interference pattern to gradually disappear, but this could be accounted for simply by random scattering, and not be due to increased decoherence caused by an increase in "which path" information. Random scattering would cause the interference pattern to disappear regardless of any effects on decoherence.
However, I also assume that the designers of the experiments were aware of this, and accounted for it somehow. I'm just wondering how. I really would like to be sure, whether or not denser mediums cause an increase in decoherence, because this would provide an important clue into the nature of the process of decoherence. So I'm actually hoping that you can clear this up for me. (Not that I'm trying to use you as my own personal assistant, sorry)
See the following excerpt(Nature, Vol.401):
"In quantum interference experiments, coherent superposition
only arises if no information whatsoever can be obtained, even in
principle, about which path the interfering particle took. Interaction
with the environment could therefore lead to decoherence.We
now analyse why decoherence has not occurred in our experiment
and how modifications of our experiment could allow studies of
decoherence using the rich internal structure of fullerenes.
In an experiment of the kind reported here, ‘which-path’ information
could be given by the molecules in scattering or emission
processes, resulting in entanglement with the environment and a
loss of interference. Among all possible processes, the following are
the most relevant: decay of vibrational excitations via emission of
infrared radiation, emission or absorption of thermal blackbody
radiation over a continuous spectrum, Rayleigh scattering, and
collisions.
When considering these effects, one should keep in mind that
only those scattering processes which allow us to determine the path
of a C60 molecule will completely destroy in a single event the
interference between paths through neighbouring slits. This
requires lpd; that is, the wavelength l of the incident or emitted
radiation has to be smaller than the distance d between neighbouring
slits, which amounts to 100nm in our experiment. When this
condition is not fulfilled decoherence is however also possible via
multi-photon scattering7,8,17.
At T < 900 K, as in our experiment, each C60 molecule has on
average a total vibrational energy of Ev < 7 eV (ref. 18) stored in 174
vibrational modes, four of which may emit infrared radiation at
lvib < 7–19mm (ref. 10) each with an Einstein coefficient of
Ak < 100 s21 (ref. 18). During its time of flight from the grating
towards the detector (t < 6 ms) a C60 molecule may thus emit on
average 2–3 such photons.
In addition, hot C60 has been observed19 to emit continuous
blackbody radiation, in agreement with Planck’s law, with a measured
integrated emissivity of e < 4:5 ð 6 2:0Þ 3 1025 (ref. 18). For
a typical value of T < 900 K, the average energy emitted during the
time of flight can then be estimated as only Ebb < 0:1 eV. This
corresponds to the emission of (for example) a single photon at
l < 10mm. Absorption of blackbody radiation has an even smaller
influence as the environment is at a lower temperature than the
molecule. Finally, since the mean free path for neutral C60 exceeds
100min our experiment, collisions with background molecules can
be neglected.
As shown above, the wavelengths involved are too large for single
photon decoherence. Also, the scattering rates are far too small to
induce sufficient phase diffusion. This explains the decoupling of
internal and external degrees of freedom, and the persistence of
interference in our present experiment."
http://atomfizika.elte.hu/akos/orak/atfsz/dualitas/fulleren.pdf