Table 3 Light-matter-interaction fits.

From: Generation of large coherent states by bang–bang control of a trapped-ion oscillator

s

Ω 0 /(2 π ) (kHz)

δ off /(2 π ) (kHz)

0

205

0

1

211

4

2

218

−4

3

224

−12

4

226

−23

5

226

−32

  1. Fit results for the light-matter-interaction experiment. The probe-pulse frequencies for sidebands s=0–2 were pre-calibrated with non-displaced states. Higher order sidebands are too weak for a direct measurement with non-displaced states, so probe-pulse frequencies for s>2 where estimated from the lower sideband frequencies. This explains the large systematic shifts in δoff resulting from the fits.
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