TY - JOUR
T1 - Measurements of the ground-state polarizabilities of Cs, Rb, and K using atom interferometry
AU - Gregoire, Maxwell D.
AU - Hromada, Ivan
AU - Holmgren, William F.
AU - Trubko, Raisa
AU - Cronin, Alexander D.
N1 - Publisher Copyright:
© 2015 American Physical Society.
PY - 2015/11/20
Y1 - 2015/11/20
N2 - We measured the ground-state static electric-dipole polarizabilities of Cs, Rb, and K atoms using a three-nanograting Mach-Zehnder atom beam interferometer. Our measurements provide benchmark tests for atomic structure calculations and thus test the underlying theory used to interpret atomic parity-nonconservation experiments. We measured αCs=4πε0×59.39(9)Å3,αRb=4πε0×47.39(8)Å3, and αK=4πε0×42.93(7)Å3. In atomic units, these measurements are αCs=401.2(7),αRb=320.1(6), and αK=290.0(5). We report ratios of polarizabilities αCs/αRb=1.2532(10),αCs/αK=1.3834(9), and αRb/αK=1.1040(9) with smaller fractional uncertainty because the systematic errors for individual measurements are largely correlated. Since Cs atom beams have short de Broglie wavelengths, we developed measurement methods that do not require resolved atom diffraction. Specifically, we used phase choppers to measure atomic beam velocity distributions, and we used electric field gradients to give the atom interference pattern a phase shift that depends on atomic polarizability.
AB - We measured the ground-state static electric-dipole polarizabilities of Cs, Rb, and K atoms using a three-nanograting Mach-Zehnder atom beam interferometer. Our measurements provide benchmark tests for atomic structure calculations and thus test the underlying theory used to interpret atomic parity-nonconservation experiments. We measured αCs=4πε0×59.39(9)Å3,αRb=4πε0×47.39(8)Å3, and αK=4πε0×42.93(7)Å3. In atomic units, these measurements are αCs=401.2(7),αRb=320.1(6), and αK=290.0(5). We report ratios of polarizabilities αCs/αRb=1.2532(10),αCs/αK=1.3834(9), and αRb/αK=1.1040(9) with smaller fractional uncertainty because the systematic errors for individual measurements are largely correlated. Since Cs atom beams have short de Broglie wavelengths, we developed measurement methods that do not require resolved atom diffraction. Specifically, we used phase choppers to measure atomic beam velocity distributions, and we used electric field gradients to give the atom interference pattern a phase shift that depends on atomic polarizability.
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U2 - 10.1103/PhysRevA.92.052513
DO - 10.1103/PhysRevA.92.052513
M3 - Article
AN - SCOPUS:84948459477
SN - 1050-2947
VL - 92
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 5
M1 - 052513
ER -