The theoretical investigation of rotating Bose-Einstein condensates has
mainly focused on the emergence of quantum vortex states and the condensed
properties of such systems. In the present work, we concentrate on other facets
by examining the impact of rotation on the ground state of weakly interacting
bosons confined in anharmonic potentials computed both at the mean-field level
and particularly at the many-body level of theory. For the many-body
computations, we employ the well-established many-body method known as the
multiconfigurational time-dependent Hartree method for bosons (MCTDHB). We
present how various degrees of fragmentation can be generated following the
breakup of the ground state densities in anharmonic traps without ramping up a
potential barrier for strong rotations. The breakup of the densities is found
to be associated with the acquisition of angular momentum in the condensate due
to the rotation. In addition to fragmentation, the presence of many-body
correlations is examined by computing the variances of the many-particle
position and momentum operators. For strong rotations, the many-body variances
become smaller than their mean-field counterparts, and one even finds a
scenario with opposite anisotropies of the mean-field and many-body variances.
Further, it is observed that for higher discrete symmetric systems of order k,
namely three-fold and four-fold symmetry, breakup to k sub-clouds and emergence
of k-fold fragmentation take place. All in all, we provide a thorough many-body
investigation of how and which correlations build up when a trapped
Bose-Einstein condensate breaks up under rotation