We investigate thermally excited, dipolar Bose-Einstein condensates.
Quasi-particle excitations of the atomic cloud cause density fluctuations which
can induce the collapse of the condensate if the inter-particle interaction is
attractive. Within a variational approach, we identify the collectively excited
stationary states of the gas which form transition states on the way to the
BEC's collapse. We analyze transition states with different m-fold rotational
symmetry and identify the one which mediates the collapse. The latter's
symmetry depends on the trap aspect ratio of the external trapping potential
which determines the shape of the BEC. Moreover, we present the collapse
dynamics of the BEC and calculate the corresponding decay rate using transition
state theory. We observe that the thermally induced collapse mechanism is
important near the critical scattering length, where the lifetime of the
condensate can be significantly reduced. Our results are valid for an arbitrary
strength of the dipole-dipole interaction. Specific applications are discussed
for the elements 52Cr, 164Dy and 168Er with which dipolar BECs
have been experimentally realized.Comment: 10 pages, 6 figure