2006 37th Meeting of the Division of Atomic, Molecular and Optical Physics
Tuesday–Saturday, May 16–20, 2006;
Knoxville, TN
Session V1: Ultracold Molecules
1:30 PM–3:54 PM,
Friday, May 19, 2006
Knoxville Convention Center
Room: Lecture Hall
Chair: Cheng Chin, University of Chicago
Abstract ID: BAPS.2006.DAMOP.V1.4
Abstract: V1.00004 : Quantum dynamics calculations on atom-diatom collisions: bosons versus fermions
3:18 PM–3:54 PM
Preview Abstract
Abstract
Author:
Jeremy M. Hutson
(Durham University)
We have obtained new potential energy surfaces and carried out
full quantum
dynamics calculations for spin-polarized Li + Li$_{2}$ [1] and K
+ K$_{2}$
[2] collisions for both bosonic and fermionic isotopes. These are
``reactive'' scattering collisions because they include all possible
arrangement channels. They are carried out in hyperspherical
coordinates
[3], which allow the full boson or fermion symmetry to be
imposed. The
potential energy surfaces are highly non-additive [4].
Our calculations give very high quenching rates for alkali dimers
in excited
vibrational states. For the \textit{low} vibrationally excited
states that we can handle
at present, we do \textit{not} see any suppression of inelastic
scattering for fermionic
atoms, even when the scattering length is large and positive. The
low-temperature inelastic rate coefficients are typically above
10$^{-10}$
cm$^{3}$ s$^{-1}$. We conclude that Pauli blocking occurs only
for molecules
formed in the highest vibrational state in the potential well.
Our results have important implications for experiments aimed at
transferring molecules to lower vibrational states. We expect
that it will
be necessary to transfer them directly to the \textit{ground}
vibrational state for them to
be long-lived. Molecules produced in any intermediate vibrational
state are
likely to be ejected from the trap very quickly.
We have also carried out calculations for mixed-isotope
collisions involving
alkali dimers [5]. For $^{7}$Li colliding with either
$^{6}$Li$_{2}$ or
$^{6}$Li$^{7}$Li, reactive scattering is possible even when the
molecule is
in its lowest rovibrational state because of the change in
zero-point
energy. For $^{7}$Li + $^{6}$Li$^{7}$Li, there is only one
reactive channel
and the reactive scattering rate is suppressed by a factor of 50
compares to
the vibrational relaxation rates.
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[1] M. T. Cvita\v{s} et al., PRL 94, 033201 (2005).
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[2] G. Qu\'{e}m\'{e}ner et al., PRA 71, 032722 (2005).
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[3] P. Sold\'{a}n et al., PRL 89, 153201 (2002).
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[4] P. Sold\'{a}n et al., PRA. 67, 054702 (2003).
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[5] M. T. Cvita\v{s} et al., PRL 94, 200402 (2005).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2006.DAMOP.V1.4