Abstract
It is well-known that molecules show electronic, vibrational, and rotational degrees of freedom. In principle, by taking into account the role of these degrees of freedom, it is possible to accurately describe chemical reactions at room temperature. However, at ultracold temperatures is necessary to go one step further and include some subtle effects on the molecular Hamiltonian. In particular, it is necessary to include the fine and hyperfine splitting of the molecular states and the interaction among them [1, 2]. The interactions emerge as a consequence of diverse couplings between the nuclear spin, molecular rotation, and electron spin [1, 2].
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Notes
- 1.
Please, note that the \(\hat {\mathbf {r}}\) stands for the unit vector of the vector position r.
- 2.
In other words, the total angular momentum of the system and its projection on a given axis is conserved.
- 3.
The term physical here denotes the fact that the scattering wave function can be always be decomposed as an incoming plane wave plus a divergent spherical wave times the amplitude of scattering.
- 4.
Polarized molecules show a preferable angular momentum projection.
- 5.
- 6.
This is equivalent to C6; however, the superscript is omitted when dealigning for spherical symmetric potentials.
- 7.
This condition is general for scattering problems. One needs to choose the initial propagation point deeply in the classical forbidden region to ensure that the wave function is null at that point.
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Pérez Ríos, J. (2020). Ultracold Molecular Collisions. In: An Introduction to Cold and Ultracold Chemistry. Springer, Cham. https://doi.org/10.1007/978-3-030-55936-6_5
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