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Deep inelastic scattering — using a twenty-first-century electron–hadron collider of sufficient energy and intensity — could teach us much more about nuclear matter at the smallest resolvable scales, as well as add to our understanding of the Higgs boson and to the search for physics beyond the standard model.

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Figure 1: Total momentum density xf(x) of partons in the proton as a function of their momentum fraction x, at Q2 = 10 GeV2 (as an example).
Figure 2: The proposed layout of the LHeC.

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Correspondence to Paul Newman or Anna Stasto.

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Newman, P., Stasto, A. Dig deeper. Nature Phys 9, 448–450 (2013). https://doi.org/10.1038/nphys2718

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