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Estimating bounds on collisional relaxation rates of spin-polarized 87Rb atoms at ultracold temperatures
Author(s) -
F. H. Mies,
Carl J. Williams,
Paul S. Julienne,
M. Krauß
Publication year - 1996
Publication title -
journal of research of the national institute of standards and technology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.202
H-Index - 59
eISSN - 2165-7254
pISSN - 1044-677X
DOI - 10.6028/jres.101.052
Subject(s) - atomic physics , relaxation (psychology) , spin (aerodynamics) , dipole , ab initio , physics , scattering , ground state , ultracold atom , quantum , quantum mechanics , social psychology , thermodynamics , psychology
We present quantum scattering calculations for the collisional relaxation rate coefficient of spin-polarized 87 Rb( f = 2, m = 2) atoms, which determines the loss rate of cold Rb atoms from a magnetic trap. Unlike the lighter alkali atoms, spin-polarized 87 Rb atoms can undergo dipolar relaxation due to both the normal spin-spin dipole interaction and a second-order spin-orbit interaction with distant electronic states of the dimer. We present ab initio calculations for the second-order spin-orbit terms for both Rb 2 and Cs 2 . The corrections lead to a reduction in the relaxation rate for 87 Rb. Our primary concern is to analyze the sensitivity of the 87 Rb trap loss to the uncertainties in the ground state molecular potentials. Since the scattering length for the a 3 Σ + u state is already known, the major uncertainties are associated with the X 1 Σ + g potential. After testing the effect of systematically modifying the short-range form of the molecular potentials over a reasonable range, and introducing our best estimate of the second-order spin-orbit interaction, we estimate that in the low temperature limit the rate coefficient for loss of Rb atoms from the f = 2, m = 2 state is between 0.4 × 10 -15 cm 3 /s and 2.4 × 10 -15 cm 3 /s (where this number counts two atoms lost per collision). In a pure condensate the rate coefficient would be reduced by 1/2.

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