Recent studies show that the non-Fermi liquid (NFL) behavior of MnSi and Fe spans over an unexpectedly broad pressure range, between the critical pressure pcpc and around 2pc2pc. In order to determine the extension of their NFL regions, we analyze the evolution of the resistivity ρ(T)∼A(p)Tnρ(T)∼A(p)Tn at higher pressures. We find that in MnSi the View the MathML sourcen=32 exponent holds below View the MathML source4.8GPa≈3pc, but it increases above that pressure. At 7.2 GPa we observe the low-temperature Fermi liquid exponent n=2n=2 whereas for View the MathML sourceT>1.5K, View the MathML sourcen=53. Our measurements in Fe show that the NFL behavior ρ∼T5/3ρ∼T5/3 extends at least up to 30.5 GPa, above the entire superconducting (SC) region. In the studied pressure range, the onset of the SC transition reduces by a factor 10 down to View the MathML sourceTconset(30.5GPa)=0.23K, while the AA—coefficient diminishes monotonically by around 50%.