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The Journal of Chemical Physics

Quantum state-dependent anion–neutral detachment processes

Saba Zia Hassan, Jonas Tauch, Milaim Kas, Markus Nötzold, Roland Wester, Matthias Weidemüller

Published Feb 8, 2022• 2 citations
Publisher

Abstract

The detachment loss dynamics between rubidium atoms (Rb) and oxygen anions (O−) are studied in a hybrid atom–ion trap. The amount of excited rubidium present in the atomic ensemble is actively controlled, providing a tool to tune the electronic quantum state of the system and, thus, the anion–neutral interaction dynamics. For a ground state Rb interacting with O−, the detachment induced loss rate is consistent with zero, while the excited state Rb yields a significantly higher loss rate. The results are interpreted via ab initio potential energy curves and compared to the previously studied Rb–OH− system, where an associative electronic detachment reactive loss process hinders the sympathetic cooling of the anion. This implies that with the loss channels closed for ground-state Rb and O− anion, this system provides a platform to observe sympathetic cooling of an anion with an ultracold heavy buffer gas.

DOI
10.1063/5.0082734

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The detachment loss dynamics between rubidium atoms (Rb) and oxygen anions (O−) are studied in a hybrid atom–ion trap. The amount of excited rubidium present in the atomic ensemble is actively controlled, providing a tool to tune the electronic quantum state of the system and, thus, the anion–neutral interaction dynamics. For a ground state Rb interacting with O−, the detachment induced loss rate is consistent with zero, while the excited state Rb yields a significantly higher loss rate. The results are interpreted via ab initio potential energy curves and compared to the previously studied Rb–OH− system, where an associative electronic detachment reactive loss process hinders the sympathetic cooling of the anion. This implies that with the loss channels closed for ground-state Rb and O− anion, this system provides a platform to observe sympathetic cooling of an anion with an ultracold heavy buffer gas.
This dissertation reports sympathetic cooling of the molecular hydroxyl anion (OH– ) via collisions with ultra cold rubidium (Rb) atoms. The anion’s translational and rotational degrees of freedom were cooled simultaneously. A new generation hybrid atom-ion trap (HAITrap) has been set up, combining an octupole radio frequency (rf) trap for ion storage and a dark-spontaneous force optical trap (darkSPOT) for Rb atoms. While the octupole rf-trap provides a large rf-field-free region decreasing rf-induced collisional heating, the darkSPOT reinforces this effect by locating the atom cloud in the center of the ion trap. The darkSPOT also enables to generate large dark state fractions, suppressing associative detachment and thus ion losses. Evidence on translational sympathetic cooling in the HAITrap was provided using two methods of kinetic thermometry: photodetachment tomography (PD) and measurements of the time of flight (ToF) distribution. The ToF analysis has shown to be more conclusive and numerical simulations validated the experimental findings qualitatively. Based on a one dimensional ToF-temperature mapping, the narrowest measured energy spread would correspond to a temperature of 35 ± 5K. Deviations from thermal distributions were observed, as predicted from a theoretical model developed by our group. Rotational sympathetic cooling was observed via state selective photodetachment (SSPD). This was performed by pre-cooling the atoms with helium buffer gas at 295K and further cooling the ions with Rb at 300 μK. SSPD thermometry yielded a 70% decrease of the anions rotational temperature after interaction with Rb. These experimental findings could have direct applications in cold collision studies, quantum control of chemical reactions or sympathetic cooling of anti-protons.
Abstract We present a theoretical investigation of reactive and non-reactive collisions of Li and Rb atoms with C 2 − molecular anions at low temperatures in the context of sympathetic cooling in hybrid trap experiments. Based on accurate potential energy surfaces for the singlet and triplet states of the Li– C 2 − and Rb– C 2 − systems, we show that the associative electronic detachment reaction is inefficient but that it occurs with a large rate for collisions involving excited states of either Li/Rb or C 2 − . We also investigate rotationally inelastic collisions in order to explore the cooling of the translational and rotational degrees of freedom of C 2 − in hybrid ion-atom traps. The effect of micromotion is taken into account by considering Tsallis distributions of collision energies. We show that the translational cooling occurs much more rapidly than rotational cooling and that the presence of excited atoms leads to losses of anions on a timescale comparable to that of rotational cooling.
We present a scheme to embed molecular anions in a gas of ultracold rubidium atoms as a route towards the preparation of cold molecular ions by collisional cooling with ultracold atoms. Associative detachment as an important loss process in collisions between OH${}^{\ensuremath{-}}$ molecules and rubidium atoms is studied. The density distribution of trapped negative ions in the multipole radio frequency trap is measured by photodetachment tomography, which allows us to derive absolute rate coefficients for the process. We define a regime where translational and internal cooling of molecular ions embedded into the ultracold atomic cloud can be achieved.
We performed calculations of the optimized structure, harmonic vibrational frequencies, and dissociation energies of RbOH and its anion, and investigate the interactions between Rb and OH${}^{\ensuremath{-}}$ leading to possible associative detachment pathways. The electron affinity of RbOH was computed to be 0.2890 eV, with a bond energy of Rb+OH${}^{\ensuremath{-}}$ half that of Rb+OH. To determine other possible charge loss pathways, the Rb+OH and Rb+OH${}^{\ensuremath{-}}$ dissociation curves were computed using coupled-cluster methods along all possible collisional angles. An adiabatic curve crossing between the neutral and charged molecule was found at the inner wall of the molecular potential curve for linear geometries. Associative detachment rates were estimated using the Langevin ion capture cross section for hydroxide. We find for $v\ensuremath{\ge}2$ an associative detachment rate of $>2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}9}$ cm3{}^{3}3s${}^{\ensuremath{-}1}$, while for v=0v=0v=0 and 1 no appreciable rate exists. This strong dependence on vibrational level suggests the ability to control the associative detachment rate directly.
Following the previous study with an extensive range of quantum calculations involving different electronic states of the BN- anion [Dulitz et al., Phys. Scripta 100, 055411 (2025)], we now extend that work by modeling the quantum dynamics of the collision cooling of its rotational states in order to investigate possible paths for bringing this molecular anion down to temperatures of a few Kelvins. This specific ionic system is of direct interest when modeling experiments in cold ion traps where He or Ar atoms can function as the chief buffer gases that drive the anions down to the low trap temperatures. We employ accurate, ab initio calculations of the potential energy surfaces for the title system in its ground electronic state, interacting with either He or Ar atoms. We then obtain a wide range of inelastic cross sections and the ensuing rate coefficients in order to model the quantum kinetics of the time evolution of the cooling steps under different temperature and trap conditions. The results are analyzed and employed to estimate the cooling efficiency paths provided by various trap arrangements for the title anion. The results show that-using either of the two investigated species-the buffer gas cooling process very efficiently brings the anions to their lowest rotational states. These findings are very promising for future applications in the field of anion laser cooling.
We present a theoretical investigation of cold reactive and nonreactive collisions of Li and Rb atoms with ${\mathrm{C}}_{2}{}^{\ensuremath{-}}$. The potential energy surfaces for the singlet and triplet states of the $\mathrm{Li}\ensuremath{-}{\mathrm{C}}_{2}{}^{\ensuremath{-}}$ and $\mathrm{Rb}\ensuremath{-}{\mathrm{C}}_{2}{}^{\ensuremath{-}}$ systems have been obtained using the CASSCF followed by ic-MRCI approach with extended basis sets. The potential energy surfaces are then used to investigate the associative detachment reaction and to calculate rotationally inelastic cross sections at low collision energies by means of the close-coupling method. The results are compared to those obtained for other anionic systems such as $\mathrm{Rb}\ensuremath{-}{\mathrm{OH}}^{\ensuremath{-}}$, and the implications for hybrid-trap experiments and sympathetic cooling experiments are explored. Furthermore, we discuss the possibility to perform Doppler thermometry on the ${\mathrm{C}}_{2}{}^{\ensuremath{-}}$ anion and investigate the collision process involving excited electronic states.