17.01.2013 Views

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Chapter 3<br />

Experimental setup<br />

LASER, subst. masc.<br />

“P<strong>la</strong>nte <strong>de</strong> <strong>la</strong> famille <strong>de</strong>s Ombellifères” (Ac. 1878–1935).<br />

Le <strong>la</strong>ser à feuilles <strong>la</strong>rges, à racine cylindrique, a <strong>de</strong>s fleurs b<strong>la</strong>nches<br />

disposées en ombelles <strong>la</strong>rges et ouvertes (PRIVAT-FOC. 1870).<br />

– Le Trésor <strong>de</strong> <strong>la</strong> Langue Française informatisé<br />

This chapter gives a brief introduction to our experimental setup.<br />

As it is already <strong>de</strong>scribed elsewhere in <strong>de</strong>tail [38, 39], I will give a brief<br />

overview and make emphasis only on the parts that have been changed.<br />

First I want to give a quick overview of the experimental procedure,<br />

to help in the general un<strong>de</strong>rstanding of the following sections. Our<br />

experiment starts with the atoms in an oven, which is heated to create a<br />

gas jet. The atoms are slowed down in a Zeeman slower, after which we<br />

capture both isotopes, 6 Li and 7 Li, in a magneto-optical trap (MOT). Using<br />

a magnetic elevator, we transfer the atoms into a Ioffe-Pritchard trap, in<br />

which we perform forced evaporative cooling on the bosonic isotope 7 Li,<br />

at the same time sympathetically cooling the fermionic isotope 6 Li. In<br />

the end, the atoms are transferred into an optical dipole trap to enable<br />

us to study them in the states that are not magnetically trappable. After<br />

another evaporative cooling stage in the optical trap we can perform our<br />

experiments, which normally take p<strong>la</strong>ce in a magnetic field around our<br />

Feshbach resonance at 83 mT. As a <strong>la</strong>st step, we switch off the optical<br />

dipole trap and let the atoms expand, taking an absorption image at the<br />

end.<br />

41

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!