We present a calculation of the pion and kaon Mellin moment $\langle x^3 \rangle$ extracted directly in lattice QCD using a three-derivative local operator. We use one ensemble of gauge configurations with two degenerate light, a strange and a charm quark () of maximally twisted mass fermions with clover improvement. The ensemble reproduces a pion mass MeV, and a kaon mass MeV. Excited-states contamination is evaluated using four values of the source-sink time separation within the range of fm. We use an operator that is free of mixing, and apply a multiplicative renormalization function calculated non-perturbatively. Our results are converted to the scheme and evolved at a scale of 2 GeV, using three-loop expressions in perturbation theory. The final values are , , and $\langle x^3 \rangle_K^{s^+}=0.075(5){\rm stat}(1){\rm syst}$, where the systematic error is the uncertainty due to excited state contamination. We combine with the two lower moments to obtain the ratios and $\langle x^3 \rangle/\langle x^2 \rangle$, as well as ratios between the pion and kaon moments. In addition, we reconstruct the -dependence of the pion and kaon PDFs via 2- and 3-parameter fits to our results. We find that the reconstruction is feasible and that our lattice data favor a large -dependence that falls as for both the pion and kaon PDFs. We integrate the reconstructed PDFs to extract the higher moments with . Finally, we compare the pion and kaon PDFs, as well as the ratios of their moments, to address the effect of SU(3) flavor symmetry breaking.

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