Comparison of Spectral Linewidths for Quantum Degenerate Bosons and Fermions

Notermans, Remy; Rengelink, R. J.; Vassen, W.

doi:10.1103/physrevlett.117.213001

Cited by 17 publications

(33 citation statements)

References 21 publications

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“…By rewriting equation 1 we can express the unknown triplet-singlet scattering length in units of the very well known triplet-triplet scattering length, a tt = +7.512(5) nm = +142.0(1) a 0 [45]. We find a ts = +82.5(5.2) a 0 , which is in agreement with our previous result of a ts = +50(10) stat (43) syst a 0 [42].…”

Section: Resultssupporting

confidence: 90%

“…At the maximum density used in the experiments (peak density n(0) ≈ 4.5 × 10 13 cm −3 or equivalently µ ≈ k B × 0.5 µK), a full width δν max ≈ 4.4 kHz is expected (see supplementary material). The additional ac-Stark shift contribution to the width [42] is negligible for the range of ODT laser wavelengths used in the final measurement campaign. Possible line-pulling effects due to the asymmetric lineshape were investigated by fitting Gaussians to simulations of the broadened lineshape but were not found to affect the fitted frequencies.…”

Section: Resultsmentioning

confidence: 94%

“…The spectroscopy laser is locked to an ultrastable laser at 1542 nm (Menlo systems) via an optical frequency comb to bridge the wavelength gap in a transfer-lock configuration [42]. The ultrastable laser serves as stable short term flywheel oscillator for the measurement.…”

Section: Methodsmentioning

confidence: 99%

“…To detect excitation of the transition, we measure the increased Penning ionization rate from the excited 2 1 S 0 atoms using a microchannel plate detector (MCP) and counter (see Methods). This detection method provides substantially better signal-to-noise ratio compared to a signal based on the loss of 2 3 S 1 atoms used previously [17,29,42]. After excitation, the remaining atoms (>90%) are dropped under gravity on another MCP detector placed 17 cm directly below the trap, producing a time-of-flight (TOF) signal.…”

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Precision spectroscopy of helium in a magic wavelength optical dipole trap

et al. 2018

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Improvements in both theory and frequency metrology of fewelectron systems such as hydrogen and helium have enabled increasingly sensitive tests of quantum electrodynamics (QED), as well as ever more accurate determinations of fundamental constants and the size of the nucleus. At the same time advances in cooling and trapping of neutral atoms have revolutionized the development of increasingly accurate atomic clocks. Here, we combine these fields to reach the highest precision on an optical tranistion in the helium atom to date by employing a Bose-Einstein condensate confined in a magic wavelength optical dipole trap. The measured transition accurately connects the ortho-and parastates of helium and constitutes a stringent test of QED theory. In addition we test polarizability calculations and ultracold scattering properties of the helium atom. Finally, our measurement probes the size of the nucleus at a level exceeding the projected accuracy of muonic helium measurements currently being performed in the context of the proton radius puzzle. 1 2 R.J. RENGELINK ET AL.In the past decades, high-precision spectroscopy measurements in atomic physics scale systems have pushed precision tests of quantum electrodynamics (QED), one of the cornerstones of the standard model of physics, ever further [1, 2] and have led to accurate determinations of fundamental constants [3][4][5][6]. Recently however, measurements of transition frequencies in muonic hydrogen (µH) have revealed a discrepancy of six standard deviations [7, 8] with respect to the accepted CODATA value for the proton charge radius. This discrepancy, which has become known as the "proton radius puzzle", has stimulated strong interest in the field, as its confirmation implies the violation of lepton universality, one of the pillars of the standard model. New experiments in atomic hydrogen [9, 10], and muonic deuterium [11] have only deepened the puzzle, prompting research into other elements such as muonic helium (µ 3,4 He + ) [12]. From these measurements the charge radii of the alpha-particle and the helion (1.68 fm resp. 1.97 fm) are projected to be determined with sub-attometer accuracy, which should be compared to high-precision experiments in electronic helium atoms or ions.QED theory of the helium atom, with two electrons more complicated than hydrogen, has seen impressive improvements in recent years, with QED corrections up to order mα 6 now evaluated [2]. Recent experiments are in good agreement [13][14][15][16][17][18][19][20] and may allow a competitive value for the fine structure constant in the near future [21][22][23][24]. The anticipated evaluation of the next highest order corrections (mα 7 ) [2] would allow the determination of the 4 He nuclear charge radius with an accuracy better than 1%. At present nuclear charge radii can already be determined differentially, i.e. with respect to 4 He, due to cancellation of higher-order terms in the isotope shift. Using this approach the radii of the exotic halo nuclei 6 He and 8 He [25,26], as well as t...

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Section: Resultssupporting

confidence: 90%

Section: Resultsmentioning

confidence: 94%

Section: Methodsmentioning

confidence: 99%

mentioning

confidence: 99%

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Precision spectroscopy of helium in a magic wavelength optical dipole trap

et al. 2018

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“…There are many experiments on the the cold and ultracold 3 He gases [19,20]. Consider a 3 He gas with the density n ≃ 1 × 10 18 m −3 [38][39][40]. The lower limit on the temperature, by the above estimation, is about 0.25µK.…”

Section: /6mentioning

confidence: 99%