2015
DOI: 10.1088/0953-4075/48/19/195004
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Absolute absorption on the potassium D lines: theory and experiment

Abstract: We present a detailed study of the absolute Doppler-broadened absorption of a probe beam scanned across the potassium D lines in a thermal vapour. Spectra using a weak probe were measured on the 4S → 4P transition and compared to the theoretical model of the electric susceptibility detailed by Zentile et al (2015) in the code named ElecSus. Comparisons were also made on the 4S → 5P transition with an adapted version of ElecSus. This is the first experimental test of ElecSus on an atom with a ground state hyper… Show more

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Cited by 20 publications
(11 citation statements)
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“…The organic coating prevents spin relaxation upon atom/wall collisions [26,27]. We recall here that the K hyperfine (hf) ground (excited) state splitting, 461.7 MHz (55.5 MHz), is smaller than the Doppler width, 773.4 MHz at 300 K. Consequently, the optical hyperfine transitions are not resolved and we observe in the co-propagating scheme a single Gaussian-like absorption profile [28], while in the counter-propagating scheme the profile is modified by saturated absorption (Fig. 2).…”
mentioning
confidence: 83%
See 1 more Smart Citation
“…The organic coating prevents spin relaxation upon atom/wall collisions [26,27]. We recall here that the K hyperfine (hf) ground (excited) state splitting, 461.7 MHz (55.5 MHz), is smaller than the Doppler width, 773.4 MHz at 300 K. Consequently, the optical hyperfine transitions are not resolved and we observe in the co-propagating scheme a single Gaussian-like absorption profile [28], while in the counter-propagating scheme the profile is modified by saturated absorption (Fig. 2).…”
mentioning
confidence: 83%
“…The two beams are then overlapped along the cell main axis with a waist of 5 mm. The maximum intensity used in this work is around 6 mW/cm 2 , corresponding to a ratio I L /I s ≈3.5 where I s =1.71 mW/cm 2 is the saturation intensity of K D 1 line [28]. The intensities as well as the polarizations of the two beams can be independently controlled by neutral density filters and waveplates.…”
mentioning
confidence: 99%
“…The most frequently used filters employ alkali metals, as these have favourable properties, including (see e.g. [134]): (i) strong principal resonance lines in the visible or near infrared part of the electromagnetic spectrum [112,202,203], (ii) simple and well-understood atomic structure and interactions with fields [65,204], and (iii) the vapour pressure of these elements allow large resonant optical rotations at modest temperatures [205]. Atomic line filters have been demonstrated in different atomic species, including Cs [61,206], Rb [201,207,208], Na [60,209] and K [210].…”
Section: Narrowband Atomic Line Filtersmentioning
confidence: 99%
“…1 (note that although it is technically easier to move only the ETC, in this case the temperature regime of the cell will be changed during the movement). About 30% of the laser power was branched to form the reference spectrum using the saturated absorption (SA) scheme (3) with 1.4-cm long potassium cell [21][22][23][24].…”
Section: Methodsmentioning
confidence: 99%