- Is a Universe with only a single fermion anomalous instead of free from anomalies?
(e.g. electron, defined through fermi statistics with exchange statistics with a gained $-1$ sign, or rotating 360 degree to get $-1$ sign on the wavefunction.)
- More generally, is a Universe with only an odd number of fermions anomalous instead of free from anomalies?
Note: In Solid State systems, it seems that the ground state always have an even number of fermions. The global symmetry properties of the system usually depend on the number of fermion $(-1)^F$, the fermion parity $\pm 1$ sign. For the whole system, we usually have $$(-1)^F=(-1)^{even}=1.$$
Is there a no-go theorem for any reason? such as (global) anomalies? What may be the constraints on the emergent gauge fields for the fermionic system?