We study the two-component boosted dark matter (DM) scenario in a neutrinophilic two-Higgs doublet model ($\nu 2$HDM), which comprises of one extra Higgs doublet with a MeV scale CP-even scalar H. This model is extended with a light ($\sim 10$~MeV) singlet scalar DM $\phi_3$, which is stabilized under the existing $Z_2$ symmetry and can only effectively annihilate through scalar $H$. As the presence of a light H modify the oblique parameters to put tight constraints on the model, introduction of vectorlike leptons (VLL) can potentially salvage the issue. These additional vector-like doublet $N$ and one vector-like singlet $\chi$ are also stabilized through the $Z_2$ symmetry. The lightest vectorlike mass eigenstate $\chi_1$ ($ \sim 100$ GeV) can be the potential second DM component of the model. Individual scalar and fermionic DM candidates have Higgs/Z mediated annihilation, restricting the fermion DM in a narrow mass region while a somewhat broader mass region is allowed for the scalar DM. In a coupled scenario, light DM $\phi_3$ gets its boost from the $\chi_1$ annihilation while the fermionic DM opens up new annihilation channel $\chi_1 \chi_1 \to \phi_3 \phi_3$: decreases the relic density. This paves way for more fermionic DM mass with under-abundant relic, a region of [35-60] GeV compared to a smaller [40-50] GeV window for the single component fermion DM. On the other hand, the $\phi_3$ resonant annihilation gets diluted due to boosting effects in kinematics, which increases the DM relic leading to a smaller allowed region. To achieve an under-abundant relic, the total DM relic will be dominated by the $\chi_1$ contribution. While there is a region with $\phi_3$ contribution dominating the total DM, the combined relic becomes over-abundant. Therefore, a sub-dominant ($\sim 5 \%$) boosted scalar is the most favorable light DM candidate to be probed for detection.
Comment: 29 pages, 10 figures, 5 tables