The Q factor is proportional to the inverse of bandwidth.
Q factor is also proportional to the inductance of the coil (L) in this circuit over the internal resistance of the coil (r_L), that is Q α L / r_L.
Then, the dynamic resistance (R_D) of the inductor-capacitor circuit is proportional to L / r_L.
From Ohm's law, this dynamic resistance is proportional to the inverse of current flowing through.
So, as the circuit seems to have a very small bandwidth, the Q factor will be very high -> L / r_L will be high -> R_D will be high -> current flowing through the parallel circuit will be low.
This is what we want at the resonant frequency, so most current goes through to the load instead.
The opposite will happen though for frequencies outside the bandwidth, that is the current in the LC circuit will be high, so the load will have far lower current than at resonance.