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Charm jets as a probe for strangeness at the future Electron-Ion Collider

Miguel ArratiaYulia FurletovaT. J. HobbsFredrick OlnessStephen J. Sekula

We explore the feasibility of the measurement of charm-jet cross sections in charged-current deep-inelastic scattering at the future Electron-Ion Collider. This channel provides clean sensitivity to the strangeness content of the nucleon in the high-x region. We estimate charm-jet tagging performance with parametrized detector simulations. We show the expected sensitivity to various scenarios for strange parton distribution functions. We argue that this measurement will be key to future QCD global analyses, so it should inform EIC detector designs and luminosity requirements.

The proposed Electron-Ion Collider (EIC), to be sited at Brookhaven National Laboratory, will offer unprecedented access to the structure of nucleons and their role in the larger structure of nuclei, the hearts of atoms. It’s still a mystery today exactly why the proton and neutron, built from three primary (“valence”) quarks and a sticky mess of gluons, results in objects whose mass is 100-200 times the sum of the constituent quarks and with spin-angular momentum precisely that of the electron, a fundamental particle.

The EIC will be the world’s first polarized electron-proton collider—meaning the “spins” of both colliding particles can be aligned in a controlled way. This will make it possible to experimentally solve the outstanding mystery of how the teeming quarks and gluons inside the proton combine their spins to generate the overall spin carried by the proton. Image Credit: Brookhaven National Laboratory.

There are many measurements to be made at the EIC. A small team of physicists at University of California at Riverside, Jefferson National Laboratory, and SMU (including yours truly) is exploring the use of certain interactions between the electron and the proton in the EIC to unlock the role of the strange quark in this structure. We’re particularly curious about what happens when the electron beam emits a charged, weak force-carrier called the “W boson” and transforms a strange quark inside the proton into a charm quark. This process results in “missing energy” from a remnant neutrino (the result of the electron emitting the W) and a jet of particles initiated by the charm quark.

A cartoon of an electron (red) interacting (“colliding”) with constituents of a nucleon in a heavy atomic nucleus. This interaction is mediated by an electrically neutral force-carrying particle, the photon; we are interested in a related interaction, where the electron exchanges a charged force carrying particle, the W boson, and morphs into a neutrino in the process. Image credit: Brookhaven National Laboratory.

Like the b-quark processes I study at the ATLAS Experiment at the LHC, charm quark jets have distinctive fingerprints that allow them to be sifted from other and more copious kinds of jets. Our team has employed some basic methodologies (well-established by experiments like ZEUS, ATLAS, and CMS) for identifying charm jets and showed that we can get a large and healthy sample of events with charm jets from the EIC.

In our first paper on the subject, we look at how this sample of charm jets could resolve tension in the inferred strange quark content of the proton from past measurements. They don’t all agree, a fact that has snapped into focus only recently thanks to new data from the LHC. We’re optimistic that the EIC will help to resolve those disagreements, and provide one of many complementary paths into nuclear structure at its most fundamental level.

In our study, we find compelling evidence that there is hope to expect enough charm jets from the process of interest to allow resolving the tension between our current picture of the strange quark in the proton. Here, were see some projected statistical uncertainties (grey band) from a “suppressed” scenario where the strange quark plays less of a role in the proton. Compare that to the blue markers, which are well-separated from the grey band and indicate the difference between the suppressed and an enhanced scenario favored by recent data from the ATLAS Experiment. Image credit: arXiv:2006.12520.

We are excited about the era of precision physics with will be unlocked by the EIC, and the potential this has for a deeper understanding of data from the “high luminosity” era of the LHC in the 2030s. It’s also an awesome group of people to work with on this evolving and growing project, and I encourage others to think about getting involved.

Meet a co-author: Miguel Arratia

Assistant Professor at UC Riverside, Miguel has expertise in experimental nuclear physics, and in particular jets as a probe of physics processes and a challenge to detector design and utilization [Learn More]

Meet a Co-author: Yulia Furletova

Yulia is a Research Scientist at Jefferson National Accelerator Laboratory and has expertise on a number of subjects, including the interaction of particle beams in accelerators, detector systems and designs, and particle identification. She has extensive experience across a number of areas key to the EIC.

Meet a Co-author: Tim Hobbs

Tim is a Post-Doctoral Researcher at SMU and is a Fellow at Jefferson Laboratory’s EIC Center. He has deep expertise in the distribution of constituents inside the proton, and especially on constraints and expectations for strange quark content.

Meet a Co-Author: Fred Olness

Fred is a Professor of Physics at SMU with expertise in both the structure of the proton and how this relates to the structure of whole nuclei. In addition to this, he has deep insights into the impact that subtle contributions from other phenomena in the quark can influence the measurement of heavier quarks in the proton.