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Experiments to Control Atom Number and Phase-Space Density in ...

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2.2 6 Lithium<br />

Lithium is the lightest of the alkali a<strong>to</strong>ms. It has three electrons, one be<strong>in</strong>g<br />

unpaired <strong>in</strong> the outer shell. There are two naturally abundant iso<strong>to</strong>pes of lithium,<br />

fermionic 6 Li (nuclear sp<strong>in</strong> I = 1) <strong>and</strong> bosonic 7 Li (nuclear sp<strong>in</strong> I = 3/2). The natural<br />

abundance of 6 Li is approximately 7.6%. The melt<strong>in</strong>g po<strong>in</strong>t of lithium is 453.69 K; the<br />

boil<strong>in</strong>g po<strong>in</strong>t lies well above all relevant temperature scales of this work at 1615 K [15].<br />

The vapor pressure of lithium is an important parameter for the experiment. In<br />

the solid <strong>and</strong> liquid phases the vapor pressure is given by [19]<br />

log10 PVsol = −54.87864− 6450.944<br />

T<br />

log10 PVliq = −10.34540− 8345.574<br />

T<br />

−0.01487480T +24.82251log 10T (2.2)<br />

−0.00008840T −0.68106log 10T. (2.3)<br />

A plot of the vapor pressure <strong>in</strong> the liquid phase is shown <strong>in</strong> figure 2.2.<br />

P<strong>to</strong>rr<br />

0.01<br />

10 4<br />

10 6<br />

10 8<br />

10<br />

450 500 550 600 650 700 750 800<br />

10<br />

Figure 2.2: Vapor pressure of liquid lithium as a function of temperature.<br />

TK<br />

The work <strong>in</strong> this dissertation is entirely performed us<strong>in</strong>g 6 Li, <strong>and</strong> thus all prop-<br />

erties given relate <strong>to</strong> this iso<strong>to</strong>pe. Table 2.2 summarizes some important physical prop-<br />

erties. A more comprehensive summary of physical properties is given <strong>in</strong> [20].<br />

5

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