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arXiv:1507.04731 · Physical Review A

Universal nonmonotonic structure in the saturation curves of magneto-optical-trap-loaded Na+ ions stored in an ion-neutral hybrid trap: Prediction and observation

R. Blümel, James E. Wells, D. S. Goodman, Jonathan M. Kwolek, W. W. Smith

Published Dec 2, 2015• 3 citations
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Abstract

We predict that the maximal, steady-state ion capacity ${N}_{s}(\ensuremath{\lambda})$ of radio-frequency (rf) traps, loaded at a rate of $\ensuremath{\lambda}$ particles per rf cycle, shows universal, nonlinear, nonmonotonic behavior as a function of loading rate $\ensuremath{\lambda}$. The shape of ${N}_{s}(\ensuremath{\lambda})$, characterized by four dynamical regimes, is universal; i.e., it is predicted to manifest itself in all types of rf traps independent of the details of their construction and independent of particle species loaded. For $\ensuremath{\lambda}\ensuremath{\ll}$ 1 (region I), as expected, ${N}_{s}(\ensuremath{\lambda})$ increases monotonically with $\ensuremath{\lambda}$. However, contrary to intuition, at intermediate $\ensuremath{\lambda}\ensuremath{\sim}1$ (region II), ${N}_{s}(\ensuremath{\lambda})$ reaches a maximum, followed by a local minimum of ${N}_{s}(\ensuremath{\lambda})$ (region III). For $\ensuremath{\lambda}\ensuremath{\gg}1$ (region IV), ${N}_{s}(\ensuremath{\lambda})$ again rises monotonically. In region IV, numerical simulations, analytical calculations, and experiments show ${N}_{s}(\ensuremath{\lambda})\ensuremath{\sim}{\ensuremath{\lambda}}^{2/3}$. We confirm our predictions both experimentally with magneto-optical-trap-loaded ${\mathrm{Na}}^{+}$ ions stored in a hybrid ion-neutral trap and numerically with the help of detailed ab initio molecular-dynamics simulations.

DOI
10.1103/physreva.92.063402

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We predict that the maximal, steady-state ion capacity Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ) of radio-frequency (rf) traps, loaded at a rate of \ensuremathλ\ensuremath{\lambda}\ensuremathλ particles per rf cycle, shows universal, nonlinear, nonmonotonic behavior as a function of loading rate \ensuremathλ\ensuremath{\lambda}\ensuremathλ. The shape of Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ), characterized by four dynamical regimes, is universal; i.e., it is predicted to manifest itself in all types of rf traps independent of the details of their construction and independent of particle species loaded. For \ensuremathλ\ensuremath≪\ensuremath{\lambda}\ensuremath{\ll}\ensuremathλ\ensuremath≪ 1 (region I), as expected, Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ) increases monotonically with \ensuremathλ\ensuremath{\lambda}\ensuremathλ. However, contrary to intuition, at intermediate \ensuremathλ\ensuremath∼1\ensuremath{\lambda}\ensuremath{\sim}1\ensuremathλ\ensuremath∼1 (region II), Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ) reaches a maximum, followed by a local minimum of Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ) (region III). For \ensuremathλ\ensuremath≫1\ensuremath{\lambda}\ensuremath{\gg}1\ensuremathλ\ensuremath≫1 (region IV), Ns(\ensuremathλ){N}_{s}(\ensuremath{\lambda})Ns​(\ensuremathλ) again rises monotonically. In region IV, numerical simulations, analytical calculations, and experiments show Ns(\ensuremathλ)\ensuremath∼\ensuremathλ2/3{N}_{s}(\ensuremath{\lambda})\ensuremath{\sim}{\ensuremath{\lambda}}^{2/3}Ns​(\ensuremathλ)\ensuremath∼\ensuremathλ2/3. We confirm our predictions both experimentally with magneto-optical-trap-loaded Na+{\mathrm{Na}}^{+}Na+ ions stored in a hybrid ion-neutral trap and numerically with the help of detailed ab initio molecular-dynamics simulations.
We present experimental measurements of the steady-state ion number in a linear Paul trap (LPT) as a function of the ion-loading rate. These measurements, taken with (a) constant Paul trap stability parameter qqq, (b) constant radio-frequency (rf) amplitude, or (c) constant rf frequency, show nonlinear behavior. At the loading rates achieved in this experiment, a plot of the steady-state ion number as a function of loading rate has two regions: a monotonic rise (region I) followed by a plateau (region II). Also described are simulations and analytical theory which match the experimental results. Region I is caused by rf heating and is fundamentally due to the time dependence of the rf Paul-trap forces. We show that the time-independent pseudopotential, frequently used in the analytical investigation of trapping experiments, cannot explain region I, but explains the plateau in region II and can be used to predict the steady-state ion number in that region. An important feature of our experimental LPT is the existence of a radial cutoff ${\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{R}}_{\mathrm{cut}}$ that limits the ion capacity of our LPT and features prominently in the analytical and numerical analysis of our LPT-loading results. We explain the dynamical origin of ${\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{R}}_{\mathrm{cut}}$ and relate it to the chaos border of the fractal of non-escaping trajectories in our LPT. We also present an improved model of LPT ion-loading as a function of time.
Providing ideal conditions for the study of ion-neutral collisions, we investigate here the properties of the saturated, steady state of a three-dimensional Paul trap, loaded from a magneto-optic trap. In particular, we study three assumptions that are sometimes made under saturated, steady-state conditions: (i) The pseudopotential provides a good approximation for the number, Ns, of ions in the saturation regime, (ii) the maximum of Ns occurs at a loading rate of approximately 1 ion per rf cycle, and (iii) the ion density is approximately constant. We find that none of these assumptions are generally valid. However, based on detailed classical molecular dynamics simulations, and as a function of loading rate and trap control parameter, we show where to find convenient dynamical regimes for ion-neutral collision experiments, or how to rescale to the pseudo-potential predictions. We also investigate the fate of the electrons generated during the loading process and present a new heating mechanism, insertion heating, that in some regimes of trapping and loading may rival and even exceed the rf-heating power of the trap.
Linear Paul traps use radio frequency fields to confine ions for long times in deep potentials. The simplicity and versatility of these devices has led to their use in a wide variety of fields, from mass spectroscopy to quantum information. Within the past fifteen years, beginning with pioneering work at UConn, Paul traps have been combined with atom traps to form hybrid atom-ion traps. Hybrid traps serve as platforms for measuring ion-atom interaction rates, sympathetically cooling atomic and molecular ions, and studying the behavior of trapped ions. This work discusses simulations, analytical theory, and experiments in a hybrid trap that show a previously unknown dynamical effect in a population of trapped ions. The steady state trapped ion number in a Paul trap is non-monotonic with the loading rate of the Paul trap. This effect is universal to both Linear and 3D Paul traps and is likely to be found in other types of ion traps as well because it is the result of the Coulomb interaction in the presence of a trap. This behavior also affects the decay of ions from the trap. Understanding the loading and decay behavior from a saturated Linear Paul trap is important for the study of ion-atom interactions in a hybrid trap when the ions lack optical transitions.
We present model-independent measurements of the excited-state population of atoms in a sodium (Na) magneto-optical trap (MOT) using a hybrid ion-neutral trap composed of a MOT and a linear Paul trap (LPT). We photoionize excited Na atoms trapped in the MOT and use two independent methods to measure the resulting ions: directly by trapping them in our LPT, and indirectly by monitoring changes in MOT fluorescence. By measuring the ionization rate via these two independent methods, we have enough information to directly determine the population of MOT atoms in the excited state. The resulting measurement reveals that there is a range of trapping-laser intensities where the excited-state population of atoms in our MOT follows the standard two-level model intensity dependence. However, an experimentally determined effective saturation intensity must be used instead of the theoretically predicted value from the two-level model. We measured the effective saturation intensity to be ${I}_{\mathrm{SE}}=22.9\ifmmode\pm\else\textpm\fi{}5.1\phantom{\rule{0.222222em}{0ex}}\mathrm{mW}/{\mathrm{cm}}^{2}$ for the type-I Na MOT and ${I}_{\mathrm{SE}}=49\ifmmode\pm\else\textpm\fi{}11\phantom{\rule{0.28em}{0ex}}\mathrm{mW}/{\mathrm{cm}}^{2}$ for the type-II Na MOT, approximately 1.7 and 3.6 times the theoretical estimate, respectively. Lastly, at large trapping-laser intensities, our experiment reveals a clear departure from the two-level model at a critical intensity that we believe is due to a state-mixing effect, the critical intensity of which can be determined by a simple power broadening model.
Long-range polarization forces between ions and neutral atoms result in large elastic scattering cross sections (e.g., $\ensuremath{\sim}\phantom{\rule{-0.16em}{0ex}}\phantom{\rule{-0.16em}{0ex}}{10}^{6}\phantom{\rule{0.28em}{0ex}}\mathrm{a}.\mathrm{u}.$ for Na\mathrm{Na}Na-Na+{\mathrm{Na}}^{+}Na+ or Na\mathrm{Na}Na-Ca+{\mathrm{Ca}}^{+}Ca+ at cold and ultracold temperatures). This suggests that a hybrid ion-neutral trap should offer a general means for significant sympathetic cooling of atomic or molecular ions. We present simion 7.0 simulation results concerning the advantages and limitations of sympathetic cooling within a hybrid trap apparatus consisting of a linear rf Paul trap concentric with a Na\mathrm{Na}Na magneto-optical trap (MOT). This paper explores the impact of various heating mechanisms on the hybrid system and how parameters related to the MOT, Paul trap, number of ions, and ion species affect the efficiency of the sympathetic cooling.
A hybrid ion-neutral trap provides an ideal system to study collisional dynamics between ions and neutral atoms. This system provides a general cooling method that can be applied to species that do not have optically accessible transitions and can also potentially cool internal degrees of freedom. The long-range polarization potentials ($V\ensuremath{\propto}\ensuremath{-}\ensuremath{\alpha}/{r}^{4}$) between ions and neutrals result in large scattering cross sections at cold temperatures, making the hybrid trap a favorable system for efficient sympathetic cooling of ions by collisions with neutral atoms. We present experimental evidence of sympathetic cooling of trapped Na+{}^{+}+ ions, which are closed shell and therefore do not have a laser-induced atomic transition from the ground state, by equal-mass cold Na atoms in a magneto-optical trap.