An anomalous particle-exchange mechanism for two isolated Bose gases merged into one

In an isolated ideal Bose system with a fixed energy, the number of microstates depends solely on the configurations of bosons in excited states, implying zero entropy for particles in the ground state. When two such systems merge, the resulting entropy is less than the sum of the individual entropies. This entropy decrease is numerically shown to arise from an effectively but anomalous exchange of particles in excited states, where $\bar{N}!\mathrm{/}({\bar{N}}_1!{\bar{N}}_2!)<1$. Here, $\bar{N}$, ${\bar{N}}_1$, and ${\bar{N}}_2$ are real decimals representing, respectively, the mean number of particles in excited states in the merged system and the two individual systems before merging, with $\bar{N}<{\bar{N}}_1+{\bar{N}}_2$.