
My latest paper, working with a team of collaborators from MIT, Duke, Mississippi State, Tel Aviv University and others, was published as an editor’s suggestion in Physical Review Letters, and has been profiled by Jefferson Lab and by Physics Magazine. It presents the first measurement of sub-threshold photo-production of the J/ψ meson from protons bound inside nuclei. The J/ψ meson is an unstable particle formed from a charm quark bound to an anti-charm quark, and has a mass about three times that of the proton. It quickly decays, and often results in a high energy electron and positron. It takes quite a bit of energy to make J/ψ mesons, and it is just barely in reach in collisions at Jefferson Lab on stationary proton targets, i.e., the accelerator exceeds the energy threshold for the reaction. When using a nucleus as a target, J/ψ mesons can be produced even with energy beneath that threshold. This is because protons inside nuclei are moving! Their own kinetic energy within the nucleus can contribute to the reaction, and be turned into mass.

Why study the J/ψ? Since it’s constituent quarks are so heavy, the primary mechanism for making one in is through a reaction called gluon exchange. The gluon is the fundamental particle that mediates the strong nuclear force. The angular distribution of J/ψ mesons turns out to be related to the spatial distribution of the gluon field within the proton.
The story gets even more interesting when looking at protons bound inside nuclei. Nuclear physicists have already known for over four decades that the motion of quarks inside bound protons is distorted compared to quarks in free protons, an observation called the “EMC Effect.” We don’t know if that distortion also happens for gluons. While our measurement isn’t conclusive, there are some suggestive hints. My collaborators and I have already proposed a longer follow up experiment to Jefferson Lab to this year’s Program Advisory Committee.












