Abstract: At ∼3.9~Ga (stellar age ∼0.6~Gyr), the young Sun was far more magnetically active than today. It launched ∼102$</sup> large, fast coronal mass ejections (CMEs) per year into a denser, more magnetized wind. We follow these eruptions to Earth's atmosphere with a semi-analytic model chain. We find that a CME launched at $v_0\sim3\text{--}4\e{3}\unit{km\,s{-1}}</sup>dissipatesΔE_k\sim6\e{25}\unit{J}asitdecelerates,anamountsetonlybyitslaunchandfinalspeeds.Diffusiveshockaccelerationconverts\sim10%ofthisenergyintosolarenergeticparticles(SEPs),whosedepositiondepthdependsmainlyonaspectralbreakenergyE_b.WeshowthatthestrongerfieldmovestheAlfveˊnsurface,insidewhichthemagneticfieldcontrolsthewind,from\sim$10--25$\,\Rsunto\sim$40--60$\,\Rsun,soCMEshocksdeliverovertentimestheparticlefluenceofflares.Becausetheforcingispoweredbydeceleration,itfollowsthemeasuredwindhistory(\dot M\propto t{-2.3})</sup>anddeclinesas\sim t{-3}.</sup>Itwas\sim$50--100 times stronger at 3.9~Ga than at 2~Ga and several hundred times today's level. This decline, strongest when the Sun was faintest, is what greenhouse solutions of the faint young Sun (FYS) problem usually impose by hand. The magnitude is small: SEP-driven $\mathrm{N_2O}addsatmostafew\unit{W\,m{-2}}</sup>toa20−−40\unit{W\,m{-2}}</sup>greenhouserequirement,andonlyifafractalorganichazeextendsitslifetime.Countingenergydepositedbelowasurvivallevelnear1 hPa,wefindtheparticlesfix\sim$$4\e{10}$--$4\e{11}\unit{mol\,N\,yr<sup>{-1}}$, which could supply prebiotic feedstock to surface pools. The largest uncertainties are Eb, the event rate, the survival depth, and the N2O lifetime.