Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Atom interferometry measurements of the polarizability of Na, K, and Rb

William F. Holmgren, Melissa Revelle, Vincent Lonij, Alexander D. Cronin

Published May 21, 2009• 0 citations
OpenAlex

Related papers

Atom interferometry measurement of the electric polarizability of lithium

Alain Miffre, Marion Jacquey, M Büchner +2 more

arXiv:quant-ph/0507279•The European Physical Journal D•Jan 16, 2006•70 citations

ANALYSIS OF ALKALI METAL ATOMIC POLARIZABILITIES AND DEVELOPING ATOM INTERFEROMETRY WITH METASTABLE HELIUM

Nathan J. Brooks

Atom interferometry is a powerful method for precision measurements of atomic properties such as polarizability, which quantifies the energy shift of an atom due to an applied electric field. In this work, we interpret recent Cs, Rb, K, and Na atomic polarizability measurements in terms of transition matrix elements, excited state lifetimes, and atomic oscillator strengths. We also use these measurements to improve calculations of van der Waals atom-atom interaction potentials. We then combine measurements of polarizability and van der Waals potentials in order to empirically quantify the e↵ect of atomic core (inner-shell) electrons on these properties. This novel method expands the utility of atom interferometry as a test for modern atomic structure calculations. In addition, we explore the possibility of extending our polarizability measurements to metastable helium atoms, for the purpose of reducing systematic errors in our existing measurements, and to strontium atoms, of interest in the construction of next-generation atomic clocks.

•Jan 1, 2016•0 citations

MEASURING POLARIZABILITY OF NA, K, AND RB WITH AN ATOM INTERFEROMETER

Melissa Revelle

•May 1, 2009•0 citations

Polarizability measurements of alkali atoms using an atom interferometer

Ivan Hromada, William F. Holmgren, Raisa Trubko +1 more

Bulletin of the American Physical Society•Jun 6, 2012•0 citations

Measurements of the ground-state polarizabilities of Cs, Rb, and K using atom interferometry

Maxwell D. Gregoire, Ivan Hromada, William F. Holmgren +2 more

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 ${\ensuremath{\alpha}}_{\mathrm{Cs}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}59.39(9)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3},{\ensuremath{\alpha}}_{\mathrm{Rb}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}47.39(8)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3}$, and ${\ensuremath{\alpha}}_{\mathrm{K}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}42.93(7)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3}$. In atomic units, these measurements are ${\ensuremath{\alpha}}_{\mathrm{Cs}}=401.2(7),{\ensuremath{\alpha}}_{\mathrm{Rb}}=320.1(6)$, and ${\ensuremath{\alpha}}_{\mathrm{K}}=290.0(5)$. We report ratios of polarizabilities ${\ensuremath{\alpha}}_{\mathrm{Cs}}/{\ensuremath{\alpha}}_{\mathrm{Rb}}=1.2532(10),{\ensuremath{\alpha}}_{\mathrm{Cs}}/{\ensuremath{\alpha}}_{\mathrm{K}}=1.3834(9)$, and ${\ensuremath{\alpha}}_{\mathrm{Rb}}/{\ensuremath{\alpha}}_{\mathrm{K}}=1.1040(9)$ 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.

arXiv:1509.07091•Physical Review A•Nov 20, 2015•78 citations

Results of Atom Interferometry Experiments with Potassium

John F. Clauser

Springer eBooks•Jan 1, 1995•0 citations
Atom interferometry is a powerful method for precision measurements of atomic properties such as polarizability, which quantifies the energy shift of an atom due to an applied electric field. In this work, we interpret recent Cs, Rb, K, and Na atomic polarizability measurements in terms of transition matrix elements, excited state lifetimes, and atomic oscillator strengths. We also use these measurements to improve calculations of van der Waals atom-atom interaction potentials. We then combine measurements of polarizability and van der Waals potentials in order to empirically quantify the e↵ect of atomic core (inner-shell) electrons on these properties. This novel method expands the utility of atom interferometry as a test for modern atomic structure calculations. In addition, we explore the possibility of extending our polarizability measurements to metastable helium atoms, for the purpose of reducing systematic errors in our existing measurements, and to strontium atoms, of interest in the construction of next-generation atomic clocks.
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 ${\ensuremath{\alpha}}_{\mathrm{Cs}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}59.39(9)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3},{\ensuremath{\alpha}}_{\mathrm{Rb}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}47.39(8)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3}$, and ${\ensuremath{\alpha}}_{\mathrm{K}}=4\ensuremath{\pi}{\ensuremath{\epsilon}}_{0}\ifmmode\times\else\texttimes\fi{}42.93(7)\phantom{\rule{0.16em}{0ex}}{\AA{}}^{3}$. In atomic units, these measurements are ${\ensuremath{\alpha}}_{\mathrm{Cs}}=401.2(7),{\ensuremath{\alpha}}_{\mathrm{Rb}}=320.1(6)$, and ${\ensuremath{\alpha}}_{\mathrm{K}}=290.0(5)$. We report ratios of polarizabilities ${\ensuremath{\alpha}}_{\mathrm{Cs}}/{\ensuremath{\alpha}}_{\mathrm{Rb}}=1.2532(10),{\ensuremath{\alpha}}_{\mathrm{Cs}}/{\ensuremath{\alpha}}_{\mathrm{K}}=1.3834(9)$, and ${\ensuremath{\alpha}}_{\mathrm{Rb}}/{\ensuremath{\alpha}}_{\mathrm{K}}=1.1040(9)$ 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.