We use all the available new precise data for deep inelastic and related hard scattering processes to perform NLO global parton analyses. These new data allow an improved determination of partons and, in particular, the inclusion of the recent measurements of the structure functions at HERA and of the inclusive jets at the Tevatron help to determine the gluon distribution and aS better than ever before. We find a somewhat smaller gluon at low x than previous determinations and that aS (MZ2) = 0.119 ±0.002 (expt.) ±0.003 (theory)
We determine the uncertainties on observables arising from the errors on the experimental data that ...
Hard processes in diffractive deep-inelastic scattering can be described by a factorisation into par...
We present LO, NLO and NNLO sets of parton distribution functions (PDFs) of the proton determined fr...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We present the new MSHT20 set of parton distribution functions (PDFs) of the proton, determined from...
AbstractWe propose a more physical parameterization of the gluon distribution for global parton anal...
The production of two-jet final states in deep inelastic scattering is an important QCD precision ob...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
Hadronic jets in deeply inelastic electron-proton collisions are produced by the scattering of a par...
We determine the uncertainties on observables arising from the errors on the experimental data that ...
Hard processes in diffractive deep-inelastic scattering can be described by a factorisation into par...
We present LO, NLO and NNLO sets of parton distribution functions (PDFs) of the proton determined fr...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We use all the available new precise data for deep inelastic and related hard scattering processes t...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
We present the new MSHT20 set of parton distribution functions (PDFs) of the proton, determined from...
AbstractWe propose a more physical parameterization of the gluon distribution for global parton anal...
The production of two-jet final states in deep inelastic scattering is an important QCD precision ob...
We perform a NNLO (and a LO) global parton analysis in which we include the new precise data for dee...
Hadronic jets in deeply inelastic electron-proton collisions are produced by the scattering of a par...
We determine the uncertainties on observables arising from the errors on the experimental data that ...
Hard processes in diffractive deep-inelastic scattering can be described by a factorisation into par...
We present LO, NLO and NNLO sets of parton distribution functions (PDFs) of the proton determined fr...