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Single-Photon Atomic Cooling - Raizen Lab - The University of ...

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the atomic ensemble. Not surprisingly and as shown in [34], the information<br />

entropy content carried away by the scattered photons is equal to the reduction<br />

in the entropy <strong>of</strong> the cooled atomic ensemble.<br />

What is really striking is how extremely efficient the single-photon cool-<br />

ing process is in using information entropy to cool. In the ideal case described<br />

above it is perfectly efficient; the reduction in entropy <strong>of</strong> the atomic ensemble<br />

equals the information entropy carried away by the spontaneously scattered<br />

photons. When compared to other established atomic laser cooling techniques,<br />

where the increase in photon entropy is typically several orders <strong>of</strong> magnitude<br />

higher than the decrease in the entropy <strong>of</strong> the atomic ensemble cooled [35], we<br />

see just how truly remarkable this process is. Additionally, single-photon cool-<br />

ing is a passive technique in the sense that one need not monitor the scattered<br />

photons at all for the process to work. In contrast, stochastic cooling methods,<br />

which like single-photon techniques scatter photons which carry information<br />

related the ensemble’s properties, must actively feedback on the data gathered<br />

from scattered photons to operate [36, 37].<br />

1.6 A Note on Units<br />

A brief discussion <strong>of</strong> the terminology and units used throughout is<br />

warranted. Of particular note is the loose manner in which the term “tem-<br />

perature” is used in the laser cooling community and indeed in this text. <strong>The</strong><br />

concept <strong>of</strong> temperature is defined in thermodynamics as a property <strong>of</strong> a closed<br />

system in thermal equilibrium with its surroundings [38, 39]. In typical atomic<br />

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