At t=0, the current through the resistance R is V/R
The ratio of the currents through L1 and L2 is fixed at all times (t>0)
After a long time, the current through L2 will be VR L1/(L1+L2)
After a long time, the current through L1 will be VR L2/(L1+L2)
L = L1L2/(L1+L2)
I = V/R(1-e^(-t/τ)), I = L1L2R/(L1+L2)
IL2 = V × L1/(L1+L2)
IL1 = V × (L2/(L1+L2))
Applying KVL -IR -LdI/dt + V = 0 → 0∫1 dI/(V-IR) = V/R(1-e^(-Rt/L))
Hence B and C are correct.