Experiments to Control Atom Number and Phase-Space Density in ...
Experiments to Control Atom Number and Phase-Space Density in ...
Experiments to Control Atom Number and Phase-Space Density in ...
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neglect the effect of the spontaneously scattered pho<strong>to</strong>n. The f<strong>in</strong>al volume Vf occupied<br />
by the gas is now dependent only on the residual <strong>in</strong>ternal energy. By reduc<strong>in</strong>g the<br />
<strong>in</strong>ternal energyUf, the f<strong>in</strong>al volumeVf will therefore also be m<strong>in</strong>imized. The efficiency of<br />
the cool<strong>in</strong>g method will therefore benefit immensely from the removal of k<strong>in</strong>etic energy<br />
from the system. Typically the spontaneously scattered pho<strong>to</strong>n can be neglected for<br />
the experiments presented <strong>in</strong> this dissertation, however, the s<strong>in</strong>gle-pho<strong>to</strong>n recoil is the<br />
fundamental limit <strong>to</strong> phase-space densities achievable by s<strong>in</strong>gle-pho<strong>to</strong>n cool<strong>in</strong>g.<br />
3.4 Maxwell’s Demon<br />
In 1867 James Clerk Maxwell proposed a gedankenexperiment commonly referred<br />
<strong>to</strong> as Maxwell’s demon [62]. In the orig<strong>in</strong>al idea a ”very observant <strong>and</strong> neat-f<strong>in</strong>gered<br />
be<strong>in</strong>g” could sort a gas of a<strong>to</strong>ms or molecules accord<strong>in</strong>g <strong>to</strong> their velocities <strong>in</strong><strong>to</strong> two<br />
separate halves of one conta<strong>in</strong>er by operat<strong>in</strong>g a massless trap door. He argued that<br />
if the demon could sense the velocity of the a<strong>to</strong>ms as they approached <strong>and</strong> sort them<br />
accord<strong>in</strong>gly, a temperature differential between the two vessels could be created without<br />
do<strong>in</strong>g any work, seem<strong>in</strong>gly violat<strong>in</strong>g the second law of thermodynamics. An illustration<br />
of Maxwell’s orig<strong>in</strong>al demon is shown <strong>in</strong> figure 3.4.<br />
A B A B<br />
Figure 3.4: Maxwell’s demon allows hot a<strong>to</strong>ms (red) <strong>to</strong> move from A <strong>to</strong> B, <strong>and</strong> cold<br />
a<strong>to</strong>ms (blue) <strong>to</strong> move from B <strong>to</strong> A. No work is done on the massless gate, but a<br />
temperature differential is created. Figure adapted from Travis Bannerman.<br />
Later on Maxwell modified the orig<strong>in</strong>al concept <strong>to</strong> a demon as illustrated <strong>in</strong><br />
figure 3.5. In this scenario a ”less <strong>in</strong>telligent” demon watches the a<strong>to</strong>ms <strong>and</strong> allows<br />
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