The ΛCDM prediction of S8 ≡ σ8(Ωm/0.3) 0.5 -where σ8 is the root mean square of matter fluctuations on a 8 h −1 Mpc scale -once calibrated on Planck CMB data is 2 − 3σ lower than its direct estimate by a number of weak lensing surveys. In this paper, we explore the possibility that the 'S8-tension' is due to a non-thermal hot dark matter (HDM) fractional contribution to the universe energy density leading to a power suppression at small-scales in the matter power spectrum. Any HDM models can be characterized by its effective mass m eff sp and its contribution to the relativistic degrees of freedom at CMB decoupling ∆N eff . Taking the specific example of a sterile particle produced from the decay of the inflaton during a matter dominated era, we find that from Planck only the tension can be reduced below 2σ, but Planck does not favor a non-zero {m eff sp , ∆N eff }. In combination with a measurement of S8 from KIDS1000+BOSS+2dfLenS, the S8-tension would hint at the existence of a particle of mass m eff sp 0.67 +0.26 −0.48 eV with a contribution to ∆N eff 0.06 ± 0.05. However, Pantheon and BOSS BAO/f σ8 data restricts the particle mass to m eff sp 0.48 +0.17 −0.36 and contribution to ∆N eff 0.046 +0.004 −0.031 . We discuss implications of our results for other canonical non-thermal HDM models-the Dodelson-Widrow model and a thermal sterile particle with a different temperature in the hidden sector. We report competitive results on such hidden sector temperature which might have interesting implications for particle physics model building, in particular connecting the S8-tension to the longstanding short baseline oscillation anomaly.