  We have dealt with the twist-4 T-even transverse momentum-dependent parton
distributions (TMDs) for the case of proton in the light-front quark-diquark
model (LFQDM). By decoding the unintegrated quark-quark correlator for the
semi-inclusive deep inelastic scattering (SIDIS), we have specifically obtained
the overlap form for the unpolarized \bigg($f_{3}^{\nu}(x, {\bf
p_\perp^2})$\bigg), longitudinally polarized \bigg($ g_{3L}^{\nu}(x, {\bf
p_\perp^2}),~h_{3L}^{\perp\nu}(x, {\bf p_\perp^2})$\bigg) and transversely
polarized \bigg( ${g}^{\nu }_{3T}(x, {\bf p_\perp^2}),~{h}^{\nu }_{3T}(x, {\bf
p_\perp^2})$ and ${h}^{\nu\perp}_{3T}(x, {\bf p_\perp^2})$\bigg) proton TMDs.
We have provided the explicit expressions for both the cases of the diquark
being a scalar or a vector. Average transverse momenta and the average square
transverse momenta for the TMDs have been calculated and the results have been
tabulated with corresponding leading twist TMDs. In addition, the value of
average transverse momentum and average square transverse momentum for TMD
${f}^{\nu }_3(x, {\bf p_\perp^2})$ has been compared with the available
light-front constituent quark model (LFCQM) results. From TMDs, we have also
obtained and discussed the transverse momentum-dependent parton distribution
functions (TMDPDFs). The model relations of the twist-4 T-even TMDs with the
available leading twist T-even TMDs have also been obtained.
