2010
DOI: 10.1088/0953-4075/43/6/065302
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RF spectroscopy in a resonant RF-dressed trap

Abstract: We study the spectroscopy of atoms dressed by a resonant radiofrequency (RF) field inside an inhomogeneous magnetic field and confined in the resulting adiabatic potential. The spectroscopic probe is a second, weak, RF field. The observed line shape is related to the temperature of the trapped cloud. We demonstrate evaporative cooling of the RF-dressed atoms by sweeping the frequency of the second RF field around the Rabi frequency of the dressing field.

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Cited by 23 publications
(34 citation statements)
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“…With these figures, the criterion µ 3D <hω z requires an atom number in the quantum gas below 10 5 , which is easy to meet while keeping a good signal to noise ratio for imaging. Moreover, this vertical oscillation frequency corresponds to a temperature of 115 nK, which can easily be reached by forcing evaporation in the dressed trap with a second, weak, rf field [30][31][32]. Both the superfluid and the thermal fractions will then be in the quasi-2D regime, which makes this trap well suited for a study of the BKT physics [11].…”
Section: A Very Anisotropic Dressed Magnetic Trapmentioning
confidence: 99%
See 1 more Smart Citation
“…With these figures, the criterion µ 3D <hω z requires an atom number in the quantum gas below 10 5 , which is easy to meet while keeping a good signal to noise ratio for imaging. Moreover, this vertical oscillation frequency corresponds to a temperature of 115 nK, which can easily be reached by forcing evaporation in the dressed trap with a second, weak, rf field [30][31][32]. Both the superfluid and the thermal fractions will then be in the quasi-2D regime, which makes this trap well suited for a study of the BKT physics [11].…”
Section: A Very Anisotropic Dressed Magnetic Trapmentioning
confidence: 99%
“…The magnetic gradient was measured previously [27]. While the rf frequency is very well known, the Rabi coupling experienced by the atoms can be measured in situ with a resolution of 0.5 kHz by rf spectroscopy [32,33]. The number of atoms remaining in the dressed trap is recorded as a function of the frequency of a second, weak, rf field, which induces resonant spin flips to an un-trapped dressed state when its frequency is equal to the Rabi coupling 0 /(2π) at the position of the atoms, see for example figure 3(b).…”
Section: Experimental Implementation and Characterizationmentioning
confidence: 99%
“…B 1 (t), has frequency ω 1 and coupling strength |Ω 1 |, with other parameters like polarization considered same as B 0 (t). In RWDS approach, as used earlier [22], the ratio of the coupling strengths is assumed to be 'relatively small' (Ω 1 /Ω 0 → 0), and hence for k = 1. An appropriate amplitude envelope G(ω) was used, which has a variable strength of the positive component ω k=+1 while having the strength of the negative component ω k=−1 zero.…”
Section: A Comparison Of Mmft With Other Approachesmentioning
confidence: 99%
“…In turn, this has resulted in the theoretical framework presented here, which is applicable to a wide range of systems dressed by multiple frequencies. Transitions in atoms in RF-dressed potentials have been calculated in previous work, though restricted to a single dressing frequency [29][30][31]. Moreover, only first-order transitions were considered in [29,30] and higher-order transitions were calculated only for selected polarizations in [31].…”
Section: Introductionmentioning
confidence: 99%