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

Characterization of three-body processes near a magnetic field induced Feshbach resonance

José Paulo D'Incao, Brett D. Esry, Chris H. Greene

Published May 30, 2008• 0 citations
OpenAlex

Related papers

Characterization of three-body processes near a magnetic field induced Feshbach resonance

James R. Macdonald Lab

•Jun 15, 2008•0 citations

Characterization of the magnetic field through the three-body loss near a narrow Feshbach resonance

Yang Chen, Shuai Peng, Hongwei Gong +3 more

The narrow $s$-wave Feshbach resonance of a $^{6}\mathrm{Li}$ Fermi gas shows strong three-body loss, which is proposed to be used to measure the minute change of a magnetic field around the resonance. However, the eddy effect will cause ultracold atom experiencing a magnetic field delay to the desired magnetic field from the current of the magnetic coils. The elimination of the eddy effect will play a key role in any experiments that are motivated to measure the magnetic field to the precision of a parts per million stability. Here, we apply a method to correct the eddy effect for precision measurement of the magnetic field. We first record the three-body loss influenced by the induced eddy effect, then we use a first-order decay model to obtain the time constant of the actual magnetic field by fitting the atom loss. This precisely determines the actual magnetic field according to the time response of the three-body loss. After that, we implement the desired magnetic field to the atoms so that we can analyze the three-body loss across the narrow Feshbach resonance. The measured magnetic-field-dependent rate of three-body loss at an ultralow temperature shows that the three-body recombination is the dominated loss mechanism near the resonance. We expect this practical method of correcting the eddy effect error of the magnetic field can be further applied to future studies of quantum few- and many-body physics near a narrow Feshbach resonance.

arXiv:2102.11470•Physical Review A•Jun 17, 2021•10 citations

Low-Energy Three-Body Recombination Near a Feshbach Resonance

O. I. Kartavtsev, J. H. Macek

Few-Body Systems•May 1, 2002•35 citations

The observation of three-body narrow resonances in ultra-cold collisions

Cheng Chin, Vladan Vuletić, Andrew J. Kerman +1 more

Summary form only given, as follows. We report on the observation of narrow resonances associated with cold cesium collisions. A loss of laser cooled atoms in a trap is induced with a laser tuned to the blue of the 6S-6P transition. Several sharp resonances, with /spl sim/kHz intrinsic linewidths, are observed as a function of an applied magnetic field. The resonances appear near magnetically tunable Feshbach resonances. We identify the collision resonances as three-body processes. We have observed both mixed resonances where the collision partners are in different states and resonances consisting of identical atoms. These resonances are promising candidates of Efimov-like states. Efimov predicted that three-body, S-wave bound states could exist near a scattering resonance regardless of whether the pair-wise interaction is attractive or repulsive. These states were first predicted to occur in nuclear scattering, but have never been seen.

Quantum Electronics and Laser Science Conference•May 12, 2000•0 citations

Magnetic Field Dependence of Inelastic Collisions Near a Feshbach Resonance

Jacob Roberts, N. R. Claussen, Simon L. Cornish +1 more

APS•Jun 1, 2000•0 citations

Magnetic Field Dependence of Ultracold Inelastic Collisions near a Feshbach Resonance

Jacob Roberts, N. R. Claussen, Simon L. Cornish +1 more

Inelastic collision rates for ultracold ${}^{85}\mathrm{Rb}$ atoms in the $F\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}2$, ${m}_{f}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}\ensuremath{-}2$ state have been measured as a function of magnetic field. At 250 gauss (G), the two- and three-body loss rates were measured to be ${K}_{2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(1.87\ifmmode\pm\else\textpm\fi{}0.95\ifmmode\pm\else\textpm\fi{}0.19)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}14}{\mathrm{cm}}^{3}/\mathrm{s}$ and ${K}_{3}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}({4.24}_{\ensuremath{-}0.29}^{+0.70}\ifmmode\pm\else\textpm\fi{}0.85)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}25}{\mathrm{cm}}^{6}/\mathrm{s}$, respectively. As the magnetic field is decreased from 250 G towards a Feshbach resonance at 155 G, the inelastic rates decrease to a minimum and then increase dramatically, peaking at the Feshbach resonance. Both two- and three-body losses are important, and individual contributions have been compared with theory.

arXiv:physics/0003027•Physical Review Letters•Jul 24, 2000•196 citations
The narrow sss-wave Feshbach resonance of a 6Li^{6}\mathrm{Li}6Li Fermi gas shows strong three-body loss, which is proposed to be used to measure the minute change of a magnetic field around the resonance. However, the eddy effect will cause ultracold atom experiencing a magnetic field delay to the desired magnetic field from the current of the magnetic coils. The elimination of the eddy effect will play a key role in any experiments that are motivated to measure the magnetic field to the precision of a parts per million stability. Here, we apply a method to correct the eddy effect for precision measurement of the magnetic field. We first record the three-body loss influenced by the induced eddy effect, then we use a first-order decay model to obtain the time constant of the actual magnetic field by fitting the atom loss. This precisely determines the actual magnetic field according to the time response of the three-body loss. After that, we implement the desired magnetic field to the atoms so that we can analyze the three-body loss across the narrow Feshbach resonance. The measured magnetic-field-dependent rate of three-body loss at an ultralow temperature shows that the three-body recombination is the dominated loss mechanism near the resonance. We expect this practical method of correcting the eddy effect error of the magnetic field can be further applied to future studies of quantum few- and many-body physics near a narrow Feshbach resonance.
Summary form only given, as follows. We report on the observation of narrow resonances associated with cold cesium collisions. A loss of laser cooled atoms in a trap is induced with a laser tuned to the blue of the 6S-6P transition. Several sharp resonances, with /spl sim/kHz intrinsic linewidths, are observed as a function of an applied magnetic field. The resonances appear near magnetically tunable Feshbach resonances. We identify the collision resonances as three-body processes. We have observed both mixed resonances where the collision partners are in different states and resonances consisting of identical atoms. These resonances are promising candidates of Efimov-like states. Efimov predicted that three-body, S-wave bound states could exist near a scattering resonance regardless of whether the pair-wise interaction is attractive or repulsive. These states were first predicted to occur in nuclear scattering, but have never been seen.
Inelastic collision rates for ultracold 85Rb{}^{85}\mathrm{Rb}85Rb atoms in the F=2F\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}2F=2, ${m}_{f}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}\ensuremath{-}2$ state have been measured as a function of magnetic field. At 250 gauss (G), the two- and three-body loss rates were measured to be ${K}_{2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(1.87\ifmmode\pm\else\textpm\fi{}0.95\ifmmode\pm\else\textpm\fi{}0.19)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}14}{\mathrm{cm}}^{3}/\mathrm{s}$ and ${K}_{3}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}({4.24}_{\ensuremath{-}0.29}^{+0.70}\ifmmode\pm\else\textpm\fi{}0.85)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}25}{\mathrm{cm}}^{6}/\mathrm{s}$, respectively. As the magnetic field is decreased from 250 G towards a Feshbach resonance at 155 G, the inelastic rates decrease to a minimum and then increase dramatically, peaking at the Feshbach resonance. Both two- and three-body losses are important, and individual contributions have been compared with theory.