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By David J. Wineland, Wayne M. ltano, James C. Bergquist, John J. Bollinger
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Extra resources for Trapped Ions and Laser Cooling II
Example text
To null the rf sidebands in all directions would likely require extra compensation electrodes. In Fig. 2, we show high-resolution scans through the Doppler-free resonance at line center and across the first upper sideband. The average integration time per point is about 10 s (160 measurement cycles). The linewidth at half maximum is approximately 30 kHz at 282 nm (or 15 kHz at 563 nm), giving a fractional resolution of about 3 x lo-". 6 Hz, the required integration time per point for the same signal-to-noise ratio of Fig.
The electric-quadrupole-allowed S-D transition and the firstresonance S - P transition are probed sequentially in order to avoid light shifts and broadening af the narrow S-D transition. Clearly resolved are the recoilless absorption resonance (carrier) and the Doppler sidebands due to the residual secular motion of the laser-cooled ion. The integration time per point is about 16 s (230 measurement cycles). S. Government Not Subject to U S . Copyright RECOILLESS OPTICAL ABSORPTION AND DOPPLER. and scanned by using the twice-frequency-shifted beam obtained by retroreflecting the first-order frequencyshifted beam back through the crystal.
30 (Springer-Verlag, New York, 1979), p. 120. 16J. L. Hall, L. Hollberg, T. Baer, and H. G. Robinson, Appl. Phys. Lett. 39, 680 (1981). 17D. J. Wineland, J. C. Bergquist, W. M. Itano, and R. E. Drullinger, Opt. Lett. 5, 245 (1980); D. J. Wineland and W. M. Itano, Phys. Lett. 82A, 75 (1981). 18H. Dehmelt, J. Phys. (Paris) Colloq. 42, (28-299 (1981). 19H. G. Dehmelt, Bull. Am. Phys. SOC. 20,60 (1975). 2oW. M. Itano and D. J. Wineland, Phys. Rev. A 24, 1364 (198 1). Happer, Rev. Phys. 44, 169 (1972).