Yeah, the stuff won’t reach us. This is due to weak Coulomb coupling to the interstellar medium (neutral and plasma phases) leading to turbulent losses and from interstellar magnetic fields that will effectively randomize the trajectories on short distance scales (relative to the length of journey in question). Even if we forgot about those effects and the effects of the even stronger interplanetary magnetic fields, any burst of low-energy ions to the earth doesn’t add new net mass to earth since such ions would become part of the gain and loss mechanisms already present for such ions (influx from solar wind, trapping in Van Allen belts, loss to atmospheric effects, etc.), and those overwhelmingly dominant processes will continue to set the equilibrium, unfazed by transient inputs.
The neutrino question is much more subtle than it looks, because an interacting neutrino doesn’t just stop in the earth like a dust mote.
First, most of the interactions of supernova neutrinos in the earth will lead to a neutrino still leaving the earth. The simplest is neutrino-electron scattering or antineutrino-electron scattering: \nu + e\rightarrow\nu+e, or the same with \bar{\nu}. The neutrino will leave some energy behind, but it will not change the rest mass of whatever it hit.
Alternatively, the neutrino can interact with a nucleus instead of an electron. In this case, the neutrino still doesn’t have to leave its rest mass behind. In particular, “neutral current” interactions (i.e., those mediated by the Z boson) will result in the neutrino just tickling the nucleus on its way through.
In cases mediated by the W boson (“charged current” interactions), you have to go isotope by isotope and separately for neutrinos and antineutrinos and separately by “flavor” to tally it all because there are energy thresholds that restrict these reactions, and these depend on the precise nuclear transitions in the reactions. This process is energetically forbidden in most cases.
For the nucleus-disturbing interactions above that can occur (both neutral- and charged-current cases), the resulting products will typically weigh some few MeV more than what you started with, finally representing some new mass.
However, a neutrino interaction can also lead to a net loss of mass. The Super-K data mentioned upthread was mostly the reaction \bar{\nu}_e + ^1\!\rm{H}\rightarrow e^- + e^+ + n (“inverse beta decay”, wherein an antineutrino converts a hydrogen nucleus to a neutron and a positron) followed by neutron capture on another hydrogen atom to make deuterium. The positron annihilates with an atomic electron, and at the end of it all you went from twice the mass of ^1\rm{H} to the mass of just ^2\rm{H}, so things are about 1.5~\rm{MeV/c}^2 lighter in the end.
As noted above, the local proton flux should not be affected.
Oof. This thread calls back to the recent “Fate of the FQ forum in light of AI” thread. My confidence is quite low in AI’s abilities to handle the nuanced questions being posed here, and my confidence is quite high that it’s answers will look sound to a cursory inspection.