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The superconducting state with the usual 2e-flux quantization formed from anormal state with 3Q charge density or loop-current order is a linearcombination of 3 different paired states with an overall gauge invariant phaseand two internal phases such that the phases in equilibrium are at $2\pi/3$with respect to each other. In the fluctuation regime of such a 3-componentsuperconductor, internal phase fluctuations are of the same class as forfrustrated classical xy-spins on a triangular lattice. The fluctuation regionis known therefore to be abnormally extended below the mean-field or theKosterlitz-Thouless transition temperature. A 6e-flux and a 4e-flux quantizedstates can be constructed which are also eigenstates of the BCS Hamiltonian andstationary points of the Ginzburg-Landau free-energy with a transitiontemperature above that of the renormalized 2e-flux quantized state. Such stateshave no internal phases and so no frustrating internal phase fluctuations.These state however cannot acquire long-range order because their free-energyis higher than the co-existing fluctuating state of 2e flux-quantization. 6e-as well as 4e- flux-quantized Little-Parks oscillations however occur in whichthe resistivity increases periodically with field above that of the2e-fluctuating state in its extended fluctuation regime, as are observed,followed at low temperatures to a condensation of the time-reversal odd2e-quantized state

Extended superconducting fluctuation region and 6e and 4e flux-quantization in a Kagome compound with a normal state of 3Q-order