QCD at the extremes
The LHC has opened a new window for studies of strong interactions which today are described remarkably well in the bulk of the phase space by Quantum Chromo Dynamics (QCD). However, there are also a number of corners in the phase space which challenge our understanding of QCD and its predictions.
At the LHC, protons are collided - composite objects consisting of quarks and gluons each carrying a momentum fraction x of their mother proton. The behavior of protons in the medium-x range is well understood and has been studied extensively e.g. at HERA and the Tevatron; here, the dynamics of the partons inside the proton are well described by the DGLAP evolution equations which are also at the heart of most modern Monte Carlo (MC) generators. We work on improving the description of high energy processes by using Transverse Momentum Dependent (TMD) parton densities, which we determined with the Parton Branching method.
QCD at the Extremes is covering different areas - we first cover the area of medium x, where we believe we have the proper theory and we compare measurements with those theory predictions. The very low x region we have already investigate by a couple of the measurements. And finally, with the high luminosity and high energy reached at the LHC run II we can investigate the up to now unexplored region of very high pt and very large x.
QCD at the Extremes is far from being understood; QCD is NOT ``bread-and-butter physics’’, serving only to describe backgrounds for searches of new physics! The LHC offers the unique possibility to test QCD at the extremes and to gain new insight into very fundamental (but by no means simple) physics.