We explore the quantum dynamics of nuclear spin relaxation
in cold
collisions of 1Σ+ molecules with structureless
atoms in an external magnetic field. To this end, we develop a rigorous
coupled-channel methodology, which accounts for rotational and nuclear
spin degrees of freedom of 1Σ+ molecules
and their interaction with an external magnetic field as well as anisotropic
atom–molecule interactions. We apply the methodology to study
the collisional relaxation of the nuclear spin sublevels of 13CO molecules immersed in a cold buffer gas of 4He atoms.
We find that nuclear spin relaxation in the ground rotational manifold
(N = 0) of 13CO occurs extremely slowly
due to the absence of direct couplings between the nuclear spin sublevels.
The rates of collisional transitions between the rotationally excited
(N = 1) nuclear spin states of 13CO are
generally much higher due to the direct nuclear spin–rotation
coupling between the states. These transitions obey selection rules,
which depend on the values of space-fixed projections of rotational
and nuclear spin angular momenta (M
N
and M
I
) for the
initial and final molecular states. For some initial states, we also
observe a strong magnetic field dependence, which can be understood
by using the first Born approximation. We use our calculated nuclear
spin relaxation rates to investigate the thermalization of a single
nuclear spin state of 13CO(N = 0) immersed
in a cold buffer gas of 4He. The calculated nuclear spin
relaxation times (T
1 ≃ 1 s at T = 1 K at a He density of 10–14 cm–3) display a steep temperature dependence decreasing
rapidly at elevated temperatures due to the increased population of
rotationally excited states, which undergo nuclear spin relaxation
at a much faster rate. Thus, long relaxation times of N = 0 nuclear spin states in cold collisions with buffer gas atoms
can be maintained only at sufficiently low temperatures (k
B
T ≪ 2B
e
), where B
e
is the rotational constant.