| People | Locations | Statistics |
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| Chatterjee, Abhijit |
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| Abdullin, S. |
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| Chatterjee, R. M. |
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| Tadel, M. |
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| Anguiano, J. |
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| Polatoz, A. |
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| Kiminsu, U. |
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| Jofrehei, A. |
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| Ambrozas, M. |
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| Kwok, K. H. M. |
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| Nogima, H. |
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| Kaestli, H. C. |
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| Bury, F. |
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| Wayne, M. |
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| Adiguzel, A. |
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| Musienko, Y. |
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| Hadley, N. J. |
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| Mal, Prolay |
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| Reichert, Joseph |
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| Cooper, S. I. |
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| Alves, G. A. |
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| Lincoln, D. |
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| Hirschauer, J. |
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| Koseyan, O. K. |
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| Droll, A. |
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Chen, M.
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (19/19 displayed)
- 2023Search for a heavy composite Majorana neutrino in events with dilepton signatures from proton-proton collisions at √s=13 TeV
- 2022Enhanced GeSn Microdisk Lasers Directly Released on Si
- 2022Search for new physics in the lepton plus missing transverse momentum final state in proton-proton collisions at √s=13 TeVcitations
- 2021Robust and Flexible Optically Active 2D Membranes Based on Encapsulation of Liquid Crystals in Graphene Oxide Pockets
- 2019Free and Bound States of Ions in Ionic Liquids, Conductivity, and Underscreening Paradoxcitations
- 2019Search for excited leptons in %5Cell%5Cell%5Cgamma$ final states in proton-proton collisions at %5Csqrt{s}$ =13 TeVcitations
- 2019Pion and kaon structure at the electron-ion collidercitations
- 2018Thermodynamic Assessment of the La-Fe-O System
- 2017Search for a heavy composite Majorana neutrino in the final state with two leptons and two quarks at %5Csqrt{s}$ =13 TeVcitations
- 2017Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at root s=13 TeVcitations
- 2016Search for massive WH resonances decaying into the l%5Cnu b%5Cbar{b}$ final state at %5Csqrt{s}$ =8 TeVcitations
- 2016Search for excited leptons in proton-proton collisions at %5Csqrt{s}$ =8 TeVcitations
- 2016Search for excited leptons in proton-proton collisions at root s=8 TeVcitations
- 2016Search for massive WH resonances decaying into the l nu b(b)over-bar final state at root s=8 TeVcitations
- 2015Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at root s = 8 TeVcitations
- 2015Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions %5Csqrt{s}=$ 8 TeVcitations
- 2013Search for anomalous production of highly boosted Z bosons decaying to mu(+)mu(-) in proton-proton collisions at root s=7 TeVcitations
- 2004NOE and PGSE NMR Spectroscopic Studies of Solution Structure and Aggregation in Metallocenium Ion-Pairscitations
- 2004Phenylxylylethane (PXE): a high-density, high-flashpoint organic liquid scintillator for applications in low-energy particle and astrophysics experiments
Places of action
article
Pion and kaon structure at the electron-ion collider
Abstract
Understanding the origin and dynamics of hadron structure and in turn that of atomic nuclei is a central goal of nuclear physics. This challenge entails the questions of how does the roughly 1GeV mass-scale that characterizes atomic nuclei appear; why does it have the observed value; and, enigmatically, why are the composite Nambu-Goldstone (NG) bosons in quantum chromodynamics (QCD) abnormally light in comparison? In this perspective, we provide an analysis of the mass budget of the pion and proton in QCD; discuss the special role of the kaon, which lies near the boundary between dominance of strong and Higgs mass-generation mechanisms; and explain the need for a coherent effort in QCD phenomenology and continuum calculations, in exa-scale computing as provided by lattice QCD, and in experiments to make progress in understanding the origins of hadron masses and the distribution of that mass within them. We compare the unique capabilities foreseen at the electron-ion collider (EIC) with those at the hadron-electron ring accelerator (HERA), the only previous electron-proton collider; and describe five key experimental measurements, enabled by the EIC and aimed at delivering fundamental insights that will generate concrete answers to the questions of how mass and structure arise in the pion and kaon, the Standard Model's NG modes, whose surprisingly low mass is critical to the evolution of our Universe.