Abstract:Very Long Baseline Atom Interferometry (VLBAI) corresponds to groundbased atomic matter-wave interferometry on large scales in space and time, letting the atomic wave functions interfere after free evolution times of several seconds or wave packet separation at the scale of meters. As inertial sensors, e.g., accelerometers, these devices take advantage of the quadratic scaling of the leading order phase shift with the free evolution time to enhance their sensitivity, giving rise to compelling experiments. With… Show more
“…This shows the relevance for experiments on large baselines [23,37,[74][75][76][77] or in microgravity [78,79]. We highlight the extrapolation for the Very Long Baseline Atom Interferometer (VL-BAI) [76,80], targeting a pulse separation time of T I = 1.2 s [81]. Here, the model describing our source gives the perspective of reaching picokelvin expansion temperatures of matter-wave lensed large atomic ensem-…”
The stability of matter-wave sensors benefits from interrogating large-particle-number atomic ensembles at high cycle rates. The use of quantum-degenerate gases with their low effective temperatures allows constraining systematic errors towards highest accuracy, but their production by evaporative cooling is costly with regard to both atom number and cycle rate. In this work, we report on the creation of cold matter-waves using a crossed optical dipole trap and shaping it by means of an all-optical matter-wave lens. We demonstrate the trade off between residual kinetic energy and atom number by short-cutting evaporative cooling and estimate the corresponding performance gain in matter-wave sensors. Our method is implemented using time-averaged optical potentials and hence easily applicable in optical dipole trapping setups.
“…This shows the relevance for experiments on large baselines [23,37,[74][75][76][77] or in microgravity [78,79]. We highlight the extrapolation for the Very Long Baseline Atom Interferometer (VL-BAI) [76,80], targeting a pulse separation time of T I = 1.2 s [81]. Here, the model describing our source gives the perspective of reaching picokelvin expansion temperatures of matter-wave lensed large atomic ensem-…”
The stability of matter-wave sensors benefits from interrogating large-particle-number atomic ensembles at high cycle rates. The use of quantum-degenerate gases with their low effective temperatures allows constraining systematic errors towards highest accuracy, but their production by evaporative cooling is costly with regard to both atom number and cycle rate. In this work, we report on the creation of cold matter-waves using a crossed optical dipole trap and shaping it by means of an all-optical matter-wave lens. We demonstrate the trade off between residual kinetic energy and atom number by short-cutting evaporative cooling and estimate the corresponding performance gain in matter-wave sensors. Our method is implemented using time-averaged optical potentials and hence easily applicable in optical dipole trapping setups.
“…after a preparation time t P = 1 s with a starting expan-359 sion velocity of 2 mm s −1 , as anticipated for the VLBAI 360 setup[76,80]. After the lens the resulting expansion ve-361 locity is 0.135 mm s −1 corresponding to an equivalent 3D 362 temperature of 200 pK.367 stimulated raman transitions, Physical Review Letters 368 67, 181 (1991).369 [2] M. Kasevich and S. Chu, Measurement of the gravita-370 tional acceleration of an atom with a light-pulse atom 371 interferometer, Appl.…”
The stability of matter-wave sensors benefits from interrogating large-particle-number atomic ensembles at high cycle rates.
The use of quantum-degenerate gases with their low effective temperatures allows constraining systematic errors towards highest accuracy, but their production by evaporative cooling is costly with regard to both atom number and cycle rate.
In this work, we report on the creation of cold matter-waves using a crossed optical dipole trap and shaping it by means of an all-optical matter-wave lens.
We demonstrate the trade off between residual kinetic energy and atom number by short-cutting evaporative cooling and estimate the corresponding performance gain in matter-wave sensors.
Our method is implemented using time-averaged optical potentials and hence easily applicable in optical dipole trapping setups.
“…These remaining terms are dominated by the finite-speedof-light effect 3Δ𝑣 0 /𝑐. The estimate for already performed UFF tests [34] was Δ𝑣 0 /𝑐 2 • 10 −11 , which is close to the uncertainty of planned experiments [92]. As such, the effect has to be subtracted for the analysis of the test.…”
Section: Eep Tests With Atom Interferometrymentioning
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