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Resolved sideband cooling
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=== Example: cooling of {{chem|Ca|+}} ions === [[File:Internal structure of Ca 40 ion with zeeman splitting.png|thumb|right|Relevant {{chem|Ca|+}} structure and light: blue - Doppler cooling; red - sideband cooling path; yellow - spontaneous decay; green - spin polarization <math>\sigma^-</math> pulses]] The energy levels relevant to the cooling scheme for {{chem|Ca|+}} ions are the S<sub>1/2</sub>, P<sub>1/2</sub>, P<sub>3/2</sub>, D<sub>3/2</sub>, and D<sub>5/2</sub>, which are additionally split by a static magnetic field to their Zeeman manifolds. Doppler cooling is applied on the dipole S<sub>1/2</sub> - P<sub>1/2</sub> transition (397 nm), however, there is about 6% probability of spontaneous decay to the long-lived D<sub>3/2</sub> state, so that state is simultaneously pumped out (at 866 nm) to improve Doppler cooling. Sideband cooling is performed on the narrow quadrupole transition S<sub>1/2</sub> - D<sub>5/2</sub> (729 nm), however, the long-lived D<sub>5/2</sub> state needs to be pumped out to the short lived P<sub>3/2</sub> state (at 854 nm) to recycle the ion to the ground S<sub>1/2</sub> state and maintain cooling performance. One possible implementation was carried out by Leibfried et al.<ref name = leibfried /> and a similar one is detailed by Roos.<ref name = roos /> For each data point in the 729 nm absorption spectrum, a few hundred iterations of the following are executed: * the ion is Doppler cooled with 397 nm and 866 nm light, with 854 nm light on as well * the ion is spin polarized to the S<sub>1/2</sub>(m=-1/2) state by applying a <math>\sigma^-</math> 397 nm light for the last few moments of the Doppler cooling process * sideband cooling loops are applied at the first red sideband of the D<sub>5/2</sub>(m=-5/2) 729 nm transition * to ensure the population ends up in the S<sub>1/2</sub>(m=-1/2) state, another <math>\sigma^-</math> 397 nm pulse is applied * manipulation is carried out and analysis is carried out by applying 729 nm light at the frequency of interest * detection is carried out with 397 nm and 866 nm light: discrimination between dark (D) and bright (S) state is based on a pre-determined threshold value of fluorescence counts Variations of this scheme relaxing the requirements or improving the results are being investigated/used by several ion-trapping groups.
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