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EGAS41 - Swansea University

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41 st EGAS CP 118 Gdańsk 2009<br />

Precision spectroscopy of the 3s-3p fine-structure doublet<br />

in Mg +<br />

V. Batteiger 1,∗ , M. Herrmann 1 , S. Knünz 1 , G. Saathoff 1 , T. Udem 1 , T.W. Hänsch 1<br />

1 Max-Planck-Institute of Quantum Optics, Hans-Kopfermann-Str. 1, D-85748 Garching,<br />

Germany<br />

∗ Corresponding author: valentin.batteiger@mpq.mpg.de,<br />

Precision spectroscopy on single trapped ions has reached tremendous accuracies by probing<br />

narrow transitions in the resolved-sideband regime [1]. However, a variety of interesting<br />

transitions may not be studied in this regime, because their transition linewidths<br />

well exceed common (secular) trap frequencies. Accurate spectroscopy is then challenging,<br />

since an interrogating laser induces detuning-dependent heating and cooling which<br />

distorts the line profile. We present both theory and experimental demonstration of a<br />

spectroscopic method (Fig.1) which overcomes these limitations and allows to observe<br />

essentially unperturbed Voigt profiles with high signal-to-noise ratio (Fig.2) [2].<br />

Figure 1: An ion chain is continuously laser cooled at one side only, a weak spectroscopy<br />

laser along the trap axis probes sympathetically cooled ions. This method allows for efficient<br />

sympathetic cooling, minimizes light shifts and background photons.<br />

3000<br />

2500<br />

2000<br />

Counts/3s<br />

1500<br />

1000<br />

500<br />

0<br />

180 200 220 240 260 280 300 320 340 360 380 400<br />

Optical Frequency - 1 072 082 630 [MHz]<br />

Figure 2: Typical line scan from a single trapped 24 Mg + ion.<br />

We deduce absolute frequency reference data for transition frequencies, isotope shifts<br />

and fine structure splittings that are in particular useful for comparison with quasar absorption<br />

spectra, to test possible space-time variations of the fine structure constant [3,4].<br />

The measurement accuracy improves previous literature values, when existing, by more<br />

than two orders of magnitude.<br />

References<br />

[1] T. Rosenband et al., Science 319, 1808 (2008)<br />

[2] M. Herrmann et al., Phys. Rev. Lett. 102, 013006 (2009)<br />

[3] J.K. Webb et al., Phys. Rev. Lett. 82, 884, (1999)<br />

[4] J.C. Berengut et al., arXiv:physics/0408017, (2006)<br />

178

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