We study the reflected entropy in (1+1)-dimensional Lifshitz field theory
whose groundstate is described by a quantum mechanical model. Starting from
tripartite Lifshitz groundstates, both critical and gapped, we derive explicit
formulas for the R\'enyi reflected entropies reduced to two adjacent or
disjoint intervals, directly in the continuum. We show that the reflected
entropy in Lifshitz theory does not satisfy monotonicity, in contrast to what
is observed for free relativistic fields. We analytically compute the full
reflected entanglement spectrum for two disjoint intervals, finding a discrete
set of eigenvalues which is that of a thermal density matrix. Furthermore, we
investigate the Markov gap, defined as the difference between reflected entropy
and mutual information, and find it to be nonvanishing, signaling irreducible
tripartite entanglement in Lifshitz groundstates. As a byproduct of our results
on reflected entropy, we provide exact formulas for two other
entanglement-related quantities, namely the computable cross-norm negativity
and the operator entanglement entropy.Comment: 34 pages, 12 figure