18 research outputs found

    Controlling collisional loss and scattering lengths of ultracold dipolar molecules with static electric fields

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    Trapped samples of ultracold molecules are often short-lived, because close collisions between them result in trap loss. We investigate the use of shielding with static electric fields to create repulsive barriers between polar molecules to prevent such loss. Shielding is very effective even for RbCs, with a relatively low dipole moment, and even more effective for molecules such as NaK, NaRb and NaCs, with progressively larger dipoles. Varying the electric field allows substantial control over the scattering length, which will be crucial for the stability or collapse of molecular Bose-Einstein condensates. This arises because the dipole-dipole interaction creates a long-range attraction that is tunable with electric field. For RbCs, the scattering length is positive across the range where shielding is effective, because the repulsion responsible for shielding dominates. For NaK, the scattering length can be tuned across zero to negative values. For NaRb and NaCs, the attraction is strong enough to support tetraatomic bound states, and the scattering length passes through resonant poles where these states cross threshold. For KAg and CsAg, there are multiple bound states and multiple poles. For each molecule, we calculate the variation of scattering length with field and comment on the possibilities for exploring new physics.Comment: 12 pages, 8 figures and 1 tabl

    Five Electronic State Beyond Born–Oppenheimer Equations and Their Applications to Nitrate and Benzene Radical Cation

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    We present explicit form of Adiabatic to Diabatic Transformation (ADT) equations and expressions of non-adiabatic coupling terms (NACTs) for a coupled five-state electronic manifold in terms of ADT angles between electronic wave functions. ADT matrices eliminate the numerical instability arising from singularity of NACTs and transform the adiabatic Schrödinger equation to its diabatic form. Two real molecular systems NO<sub>3</sub> and C<sub>6</sub>H<sub>6</sub><sup>+</sup> (Bz<sup>+</sup>) are selectively chosen for the demonstration of workability of those equations. We examine the NACTs among the lowest five electronic states of the NO<sub>3</sub> radical [X̃<sup>2</sup>A<sub>2</sub><sup>′</sup> (1<sup>2</sup>B<sub>2</sub>), Ã<sup>2</sup>E″ (1<sup>2</sup>A<sub>2</sub> and 1<sup>2</sup>B<sub>1</sub>) and B̃<sup>2</sup>E′ (1<sup>2</sup>A<sub>1</sub> and 2<sup>2</sup>B<sub>2</sub>)], in which all types of non-adiabatic interactions, that is, Jahn–Teller (JT) interactions, Pseudo Jahn–Teller (PJT) interactions, and accidental conical intersections (CIs) are present. On the other hand, lowest five electronic states of Bz<sup>+</sup> [X̃<sup>2</sup>E<sub>1g</sub> (1<sup>2</sup>B<sub>3g</sub> and 1<sup>2</sup>B<sub>2g</sub>), B̃<sup>2</sup>E<sub>2g</sub> (1<sup>2</sup>A<sub>g</sub> and 1<sup>2</sup>B<sub>1g</sub>), and C̃<sup>2</sup>A<sub>2u</sub> (1<sup>2</sup>B<sub>1u</sub>)] depict similar kind of complex feature of non-adiabatic effects. For NO<sub>3</sub> radical, the two components of degenerate in-plane asymmetric stretching mode are taken as a plane of nuclear configuration space (CS), whereas in case of Bz<sup>+</sup>, two pairs are chosen: One is the pair of components of degenerate in-plane asymmetric stretching mode, and the other one is constituted with one of the components each from out-of-plane degenerate bend and in-plane degenerate asymmetric stretching modes. We calculate ab initio adiabatic potential energy surfaces (PESs) and NACTs among the lowest five electronic states at the CASSCF level using MOLPRO quantum chemistry package. Subsequently, the ADT is performed using those newly developed equations to validate the positions of the CIs, evaluate the ADT angles and construct smooth, symmetric, and continuous diabatic PESs for both the molecular systems

    Feshbach resonances and molecule formation in ultracold mixtures of Rb and Yb(3P) atoms

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    We have investigated magnetically tunable Feshbach resonances in ultracold collisions of Rb with Yb in its metastable 3P2 and 3P0 states, using coupled-channel scattering and bound-state calculations. For the 3P2 state, we find sharp resonances when both atoms are in their lowest Zeeman sublevels. However, these resonances are decayed by inelastic processes that produce Yb atoms in 3P1 and 3P0 states. The molecules that might be produced by magnetoassociation at the 3P2 thresholds can decay by similar pathways and would have lifetimes no more than a few microseconds. For the 3P0 state, by contrast, there are resonances that are promising for magnetoassociation. There are resonances due to both rotating and nonrotating molecular states that are significantly stronger than the analogous resonances for Yb(1S). The ones due to rotating states are denser in magnetic field; in contrast to Yb(1S), they exist even for bosonic isotopes of Yb(3P0)

    Non-adiabatic coupling as a frictional force in the formation of H

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    By treating the non-adiabatic coupling terms (NACTs) in a molecular system as equivalent to a frictional force, the classical equation of motion is solved for a test case of quasi-H3+ {\mathrm{H}}_3^{+} along the C2v axis and axes parallel to it, and it is shown that the singular NACTs between the first two excited electronic states slow down the relative motion of the three quasi-ions (H,H,H)+ while approaching each other
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