1999
DOI: 10.1038/23655
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Measurement of gravitational acceleration by dropping atoms

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Cited by 850 publications
(957 citation statements)
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“…The magnetic field necessary to shift adjacent Zeeman sublevels by an amount equal to the vibrational energy splitting is B max Ϸ 140 mG in the center and B min Ϸ 11 mG at the edge of the laser beam. 3 The experimental optimum lies between these upper and lower bounds.…”
Section: A Optimum Magnetic Fieldmentioning
confidence: 99%
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“…The magnetic field necessary to shift adjacent Zeeman sublevels by an amount equal to the vibrational energy splitting is B max Ϸ 140 mG in the center and B min Ϸ 11 mG at the edge of the laser beam. 3 The experimental optimum lies between these upper and lower bounds.…”
Section: A Optimum Magnetic Fieldmentioning
confidence: 99%
“…6. 3 The Zeeman frequency shift of adjacent magnetic sublevels is 350 kHz/ G for the hyperfine ground states of cesium.…”
Section: E Model Of Sideband Raman Cooling In the Lamb-dicke Regimementioning
confidence: 99%
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“…In particular, atom interferometers are new tools for experimental gravitation as, for example, for precision measurement of gravity acceleration [15], gravity gradients [16], Newtonian gravitational constant G [17], gravity at micrometric distances [18,19], and for testing equivalence principle [20]. The possibility of detecting gravitational waves by atom interferometry was also discussed [21,22].…”
Section: Atom Interferometry Sensors For Space Applicationsmentioning
confidence: 99%
“…During the past decades, atom interferometry experiments were developed for various applications like precision measurement of fundamental constants [1,2], gravimetry [3], gradiometry [4] or inertial sensing [5,6]. Based on this methods, cold atoms sensors measure interferometrically the inertial effects affecting the experiment with respect to free falling laser-cooled atoms that are split and recombined using two counter-propagating laser beams.…”
Section: Introductionmentioning
confidence: 99%