Martin Teichmann Atomes de lithium-6 ultra froids dans la ... - TEL
Martin Teichmann Atomes de lithium-6 ultra froids dans la ... - TEL
Martin Teichmann Atomes de lithium-6 ultra froids dans la ... - TEL
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Chapter 4<br />
Data analysis<br />
A correct data analysis is crucial to every experiment. In experiments on<br />
cold atoms, the raw data is normally the <strong>de</strong>nsity distribution of the atoms<br />
acquired using absorption imaging techniques. Most often, the total<br />
number of the atoms and the extent of the cloud in the two directions is<br />
sufficient to interpret the data and can be achieved easily by performing<br />
an appropriate fit on the atomic distribution. Here we want to focus<br />
on a more advanced method of data analysis: firstly, the shape of the<br />
cloud contains important information about the temperature of the cloud,<br />
which can be extracted using appropriate fitting functions. Secondly,<br />
the cloud we see on the computer screen is only a two dimensional<br />
projection. Knowing that the original cloud has rotational symmetry, we<br />
can reconstruct the three dimensional distribution of the atoms.<br />
4.1 Determination of the temperature of a fermionic<br />
gas<br />
The temperature of a c<strong>la</strong>ssical gas in a trap can be <strong>de</strong>termined easily:<br />
after a time-of-flight expansion, the momentum distribution of the gas<br />
is known from which the temperature can be easily calcu<strong>la</strong>ted. The<br />
case of a bosonic gas is very different: once the gas has con<strong>de</strong>nsed<br />
into a Bose-Einstein-Con<strong>de</strong>nsate, the fraction of the non-con<strong>de</strong>nsed<br />
atoms is directly re<strong>la</strong>ted to the temperature of the gas. At very low<br />
temperatures, the con<strong>de</strong>nsate becomes nearly pure, and a temperature<br />
measurement becomes a task that is difficult to accomplish. The case<br />
of a fermionic gas is as tricky. At low temperatures, especially below<br />
the Fermi temperature, the momentum distribution shows no changes<br />
except that the smearing of the step in the Fermi distribution.<br />
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