On this webpage, we collect calculations of the L2 sensitivities for the experiments fitted in the CT18 global QCD analysis [arXiv:1912.10053]. The L2 sensitivity reliably approximates the variation in χ2 for a given experiment when the parton distribution function (PDF), f(x,Q), for a particular parton flavor, f, is increased by one PDF uncertainty (defined at the 90% C.L.) at a specific value of (x,Q). This method can be used for both Hessian and Monte Carlo PDF error sets, and can be computed very quickly, unlike the complementary Lagrange Multiplier (LM) scans, which are computationally expensive. The L2 sensitivities can therefore be evaluated for many PDF flavors and combinations across a wide range of (x,Q) values. This can be done for all fitted experiments in a way that delivers a comprehensive view of the experimental pulls on the PDFs, as well as possible tensions among them. These tensions are realized in the L2 sensitivity plots shown below as peaks in opposing directions (i.e., ±Δχ2) at similar values of x and Q.
We present two families of L2 sensitivity plots, for the CT18 and CT18Z PDF analyses. For each of these, we show the sensitivities for various PDF flavors experiment-by-experiment, as well as the pulls of the most sensitive experiments on specific PDF flavors and combinations.
![]() Glue-glue: [pdf] |
![]() Quark-glue: [pdf] |
![]() Quark-antquark: [pdf] |
![]() Quark-quark: [pdf] |
![]() g(x,Q=2 GeV): [pdf] |
![]() u(x,Q=2 GeV): [pdf] |
![]() ub(x,Q=2 GeV): [pdf] |
![]() d(x,Q=2 GeV): [pdf] |
![]() db(x,Q=2 GeV): [pdf] |
![]() s(x,Q=2 GeV): [pdf] |
![]() c(x,Q=2 GeV): [pdf] |
![]() uval(x,Q=2 GeV): [pdf] |
![]() dval(x,Q=2 GeV): [pdf] |
![]() d/u(x,Q=2 GeV): [pdf] |
![]() db/ub(x,Q=2 GeV): [pdf] |
![]() (s+sb)/(ub+db)(x,Q=2 GeV): [pdf] |
![]() (s+sb)/(2db)(x,Q=2 GeV): [pdf] |
![]() (c+cb)/(ub+db)(x,Q=2 GeV): [pdf] |
![]() (u*db)/(d*ub)(x,Q=2 GeV): [pdf] |
![]() (u+ub-d-db)(x,Q=2 GeV): [pdf] |
![]() g(x,Q=100 GeV): [pdf] |
![]() u(x,Q=100 GeV): [pdf] |
![]() ub(x,Q=100 GeV): [pdf] |
![]() d(x,Q=100 GeV): [pdf] |
![]() db(x,Q=100 GeV): [pdf] |
![]() s(x,Q=100 GeV): [pdf] |
![]() c(x,Q=100 GeV): [pdf] |
![]() uval(x,Q=100 GeV): [pdf] |
![]() dval(x,Q=100 GeV): [pdf] |
![]() d/u(x,Q=100 GeV): [pdf] |
![]() db/ub(x,Q=100 GeV): [pdf] |
![]() (s+sb)/(ub+db)(x,Q=100 GeV): [pdf] |
![]() (s+sb)/(2db)(x,Q=100 GeV): [pdf] |
![]() (c+cb)/(ub+db)(x,Q=100 GeV): [pdf] |
![]() (u*db)/(d*ub)(x,Q=100 GeV): [pdf] |
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![]() Glue-glue: [pdf] |
![]() Quark-glue: [pdf] |
![]() Quark-antquark: [pdf] |
![]() Quark-quark: [pdf] |
![]() g(x,Q=2 GeV): [pdf] |
![]() u(x,Q=2 GeV): [pdf] |
![]() ub(x,Q=2 GeV): [pdf] |
![]() d(x,Q=2 GeV): [pdf] |
![]() db(x,Q=2 GeV): [pdf] |
![]() s(x,Q=2 GeV): [pdf] |
![]() c(x,Q=2 GeV): [pdf] |
![]() uval(x,Q=2 GeV): [pdf] |
![]() dval(x,Q=2 GeV): [pdf] |
![]() d/u(x,Q=2 GeV): [pdf] |
![]() db/ub(x,Q=2 GeV): [pdf] |
![]() (s+sb)/(ub+db)(x,Q=2 GeV): [pdf] |
![]() (s+sb)/(2db)(x,Q=2 GeV): [pdf] |
![]() (c+cb)/(ub+db)(x,Q=2 GeV): [pdf] |
![]() (u*db)/(d*ub)(x,Q=2 GeV): [pdf] |
![]() (u+ub-d-db)(x,Q=2 GeV): [pdf] |
![]() g(x,Q=100 GeV): [pdf] |
![]() u(x,Q=100 GeV): [pdf] |
![]() ub(x,Q=100 GeV): [pdf] |
![]() d(x,Q=100 GeV): [pdf] |
![]() db(x,Q=100 GeV): [pdf] |
![]() s(x,Q=100 GeV): [pdf] |
![]() c(x,Q=100 GeV): [pdf] |
![]() uval(x,Q=100 GeV): [pdf] |
![]() dval(x,Q=100 GeV): [pdf] |
![]() d/u(x,Q=100 GeV): [pdf] |
![]() db/ub(x,Q=100 GeV): [pdf] |
![]() (s+sb)/(ub+db)(x,Q=100 GeV): [pdf] |
![]() (s+sb)/(2db)(x,Q=100 GeV): [pdf] |
![]() (c+cb)/(ub+db)(x,Q=100 GeV): [pdf] |
![]() (u*db)/(d*ub)(x,Q=100 GeV): [pdf] |
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