Max Klein HERA-LHeC Manchester 31/1/08 Deep Inelastic ep Scattering at High Energies Max Klein University of Liverpool H1 and ATLAS From the Hoch-Energie-Ring-Anlage.

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Max Klein HERA-LHeC Manchester 31/1/08 Deep Inelastic ep Scattering at High Energies Max Klein University of Liverpool H1 and ATLAS From the Hoch-Energie-Ring-Anlage to the Large Hadron electron Collider 3 Seminar at the University of Manchester, January 30 th, 2008

Max Klein HERA-LHeC Manchester 31/1/08 The GeV Energy Scale [ ] Quarks Neutral currents Singlet e R Asymptotic Freedom Drell Yan Charm W,Z Jets Charm 3 colours Gluon Jets lh e+e-e+e- pp SU(2) L x U(1) QCD (--)

Max Klein HERA-LHeC Manchester 31/1/08 HERA and experiments

Max Klein HERA-LHeC Manchester 31/1/08 HERA’s last day HERA did end with a 3 month operation at reduced proton beam energies in order to measure the longitudinal proton structure function directly, which provides a crucial test of QCD at higher orders and an independent measure of the gluon density at low x.

Max Klein HERA-LHeC Manchester 31/1/08 HERA Performance HERA I : HERA II: FLFL Two years of fight for HERA’s existence (2002/2003) in what was called ‘upgrade’..

Max Klein HERA-LHeC Manchester 31/1/08 The most puzzling observation (for long) H1+ZEUS

Max Klein HERA-LHeC Manchester 31/1/08 The most spectacular fluctuation EPS07

Max Klein HERA-LHeC Manchester 31/1/08 Weak and Electromagnetic Interactions A major question in the early 80ies, would the weak and the electro- magnetic interactions “unify”?

Max Klein HERA-LHeC Manchester 31/1/08 Subsubstructure of matter?

Max Klein HERA-LHeC Manchester 31/1/08 A new phase of matter (high parton densities and small coupling)

Max Klein HERA-LHeC Manchester 31/1/08 The beautiful f2 Low x is gluon dominated HERA very precise in the LHC rapidity plateau region You can never have enough luminosity at high x and Q2 H1&ZEUS now cooperate really

Max Klein HERA-LHeC Manchester 31/1/08 NC

Max Klein HERA-LHeC Manchester 31/1/08 The knowledge of the pdfs (HERA) is crucial for LHC

Max Klein HERA-LHeC Manchester 31/1/08 averaging

Max Klein HERA-LHeC Manchester 31/1/08 Electroweak Measurements at HERA

Max Klein HERA-LHeC Manchester 31/1/08 Light quark couplings

Max Klein HERA-LHeC Manchester 31/1/08 Beauty density

Max Klein HERA-LHeC Manchester 31/1/08 Hard Diffraction at HERA U.Klein /

Max Klein HERA-LHeC Manchester 31/1/08 MANY more important results from HERA Hard Diffraction (the return of the IP) Vector Mesons Deeply Virtual Compton Scattering (Parton Amplitudes!) Transverse Size of the Gluon Charm Structure Function Jets Strong Coupling “Constant” Low x Parton Dynamics (“fwd jets”, azimuthal decorr.’s) Pion Structure Function Partonic Structure of the Photon … HERA has delivered much more than was expected. The final results are being worked on (+3 years)

Max Klein HERA-LHeC Manchester 31/1/08 The Fermi Scale [ ] b quark top quark M W gluon h.o. strong c,b distributions high parton densities M Z, sin 2  3 neutrinos h.o. el.weak (t,H?) ep e+e-e+e- pp The Standard Model Triumph Tevatron LEP/SLC HERA CKM - B factories

Max Klein HERA-LHeC Manchester 31/1/08 The TeV Scale [ ] W,Z,top Higgs?? New Particles?? New Symmetries? High Precision QCD High Density Matter Substructure?? eq-Spectroscopy?? ttbar Higgs?? Spectroscopy?? ep e+e-e+e- pp New Physics LHC ILC/CLIC LHeC Predicting is difficult, in particular if it concerns the future.

Max Klein HERA-LHeC Manchester 31/1/08 Physics and Range High mass 1-2 TeV r q few times m High precision partons in plateau of the LHC Nuclear Structure & dynamics High Density Matter Large x Former considerations: ECFA Study J.Feltesse, R.Rueckl: Aachen Workshop (1990) The THERA Book (2001)& Part IV of TESLA TDR Phys. working groups New Physics QCD+electroweak High parton densities

Max Klein HERA-LHeC Manchester 31/1/08 New Physics - Electron-Quark Resonances Appear in many extensions of the SM, e.g. RP violating SUSY. Scalar or vector colour triplet bosons Symmetry between q and l sector. B, L violation? Could be discovered via pair production at LHC up to masses of TeV Charge, angular distribution, polarisation: quantum numbers may be determined in ep. Similarly: If the LHC sees some CI, you may need pp and ep and ee to resolve the new i.a.. SM: A.Zarnecki

Max Klein HERA-LHeC Manchester 31/1/08 Quantum Numbers Charge asymmetry much cleaner in ep than in pp. Similar for simultaneous determination of coupling and quark flavour E.Perez, DIS07

Max Klein HERA-LHeC Manchester 31/1/08 xg Gluon Beauty b hep-ph/ , Belyayev et al Higgs <-SM MSSM->

Max Klein HERA-LHeC Manchester 31/1/08 Complete Unfolding of the Quark Content of the Nucleon (NC,CC) at PeV energies d (d/u) at large x valence at small x also W+- at LHC strange and antistrange from charged currents for the first time precision charm

Max Klein HERA-LHeC Manchester 31/1/08 Strong Coupling Detector Requirements The strong coupling constant is the worst of all measured couplings. The LHeC leads to a per mille level of exp. accuracy, a new challenge to pert. and lattice QCD. T.Kluge, MK, DIS07

Max Klein HERA-LHeC Manchester 31/1/08 Stan Brodsky’s 13 Questions Multijets: fwd jets, low x, LHC Heavy flavours & hadron structure QCD - a rich theory

Max Klein HERA-LHeC Manchester 31/1/08 Neutron Structure (ed  eX) crucial constraint on evolution (S-NS), improved  s

Max Klein HERA-LHeC Manchester 31/1/08 Nuclear Structure extension of x range by 4 orders of magnitude and huge extension in Q 2 unitarity limit

Max Klein HERA-LHeC Manchester 31/1/08 LHC An electron ring would have to bypass experiments. P3 and 6, perhaps An electron linac would be largely decoupled from the LHC. In any case, an ep/eA interaction region by then would have to be in P2 or/and P8.

Max Klein HERA-LHeC Manchester 31/1/08 Luminosity: Ring-Ring can be reached in RR E e = GeV & P = 5-60 MW. HERA was cm -2 s -1 huge gain with SLHC p beam F.Willeke in hep-ex/ : Design of interaction region for : 50 MW, 70 GeV May reach with ERL in bypasses, or/and reduce power. R&D performed at BNL/eRHIC  I e = 100 mA likely klystron installation limit Synchrotron rad! cf also A.Verdier 1990, E.Keil 1986

Max Klein HERA-LHeC Manchester 31/1/08 Luminosity: Linac-Ring LHeC as Linac-Ring version can be as luminous as HERA II: can be reached with LR: E e = GeV & P=20-60 MW LR: average lumi close to peak 140 GeV at 23 MV/m is 6km +gaps Luminosity horizon: high power: ERL (2 Linacs?)  I e = 100 mA High cryo load to CW cavities

Max Klein HERA-LHeC Manchester 31/1/08 Ring-Ring LHeC Interaction Region Design foresees simultaneous operation of pp and ep

Max Klein HERA-LHeC Manchester 31/1/08 Design Details First p beam lens: septum quadrupole. Cross section and Field calculation Synchrotron radiation fan and HERA type absorber 100W/mm 2 cf also W.Bartel Aachen 1990

Max Klein HERA-LHeC Manchester 31/1/08 Accelerator (RR) questions considered Power: 25ns: nx40MHz rf frequency. Imax 100 mA: 60 klystrons with 1.3MW coupler of perhaps 0.5MW, 66% efficient… need space for rf in bypasses Injection: LEP2 was N= in 4 bunches, LHeC is in 2800 bunches may inject at less than 20 GeV. Injection is no principal problem regarding power and technology (ELFE, KEK, direct?) Synchrotron load to LHC magnets: can be shielded (water cooled Pb) Bypasses: for ATLAS and CMS but also for further Pi. l~500m start in the arcs. May ensure same length of e ring as p with ~ -20cm radius of e ring. Space: first look at the installation on top of LHC

Max Klein HERA-LHeC Manchester 31/1/08 Circulating LHC beams pass in between support feet Kicker magnet installed on beam dump line above LHC Passing equipment above installed LHC beamlines….

Max Klein HERA-LHeC Manchester 31/1/08 e ± Linac - p/A Ring alternative sites 6km S. Chattopadhyay (Cockcroft), F.Zimmermann (CERN), et al.

Max Klein HERA-LHeC Manchester 31/1/08 Comparison Linac-Ring and Ring-Ring Energy / GeV Luminosity / cm -2 s Mean Luminosity, relative 2 1 [dump at L peak /e] Lepton Polarisation 60-80% 30% [?] Tunnel / km 6 2.5=0.5 * 5 bypasses Biggest challenge CW cavities Civil Engineering Ring+Rf installation Biggest limitation luminosity (ERL,CW) maximum energy IR not considered yet allows ep+pp one design? (eRHIC) 2 configurations [lox, hiq]

Max Klein HERA-LHeC Manchester 31/1/08 DIS events 100 fb GeV 1 fb -1 HERA (sim) The strong decrease of the DIS cross section with Q 2 requires highest possible luminosity. Statistics at LHeC for up to ~10 5 GeV 2 is rich. No statistics problem for low x physics - two versions of IR and instrumentation possible, though not really desired. Highest scales: large energy counts for discovery range. Neutral Currents ep ->eX Charged Currents ep -> X 10 fb GeV The LHeC is a huge step from HERA into the TeV range. At very large Q 2 10 times less L is compensated by 2 E e.

Max Klein HERA-LHeC Manchester 31/1/08 The Goal of the ECFA-CERN Workshops is a CDR by end of 2009: Accelerator Design [RR and LR] Closer evaluation of technical realisation: injection, magnets, rf, power efficiency, cavities, ERL… What are the relative merits of LR and RR? Recommendation. Interaction Region and Forward Detectors Design of IR (LR and RR), integration of fwd detectors into beam line. Infrastructure Definition of infrastructure - for LR and RR. Detector Design A conceptual layout, including alternatives, and its performance [ep and eA]. New Physics at Large Scales Investigation of the discovery potential for new physics and its relation to the LHC and ILC/CLIC. Precision QCD and Electroweak Interactions Quark-gluon dynamics and precision electroweak measurements at the TERA scale. Physics at High Parton Densities [small x and eA] QCD and Unitarity, QGP and the relations to nuclear, pA/AA LHC and SHE physics.

Max Klein HERA-LHeC Manchester 31/1/08 Scientific Advisory Committee (SAC) Accelerator Experts S.Chattopadhyay, R.Garoby, S.Myers, A. Skrinsky, F.Willeke Research Directors+ECFA J.Engelen, R.Heuer, Y-K.Kim P.Bond, K.H.Meier Theorists G.Altarelli, S.Brodsky, J.Ellis, L.Lipatov, F. Wilczek Experimentalists A.Caldwell (chair), J.Dainton, J.Feltesse, R.Horisberger, A.Levy, R.Milner

Max Klein HERA-LHeC Manchester 31/1/08 Steering Group Oliver Bruening (CERN) John Dainton (Cockcroft) Albert DeRoeck (CERN) Stefano Forte (Milano) Max Klein - chair (Liverpool) Paul Newman (Birmingham) Emmanuelle Perez (CERN) Wesley Smith (Wisconsin) Bernd Surrow (MIT) Katsuo Tokushuku (KEK) Urs Wiedemann (CERN) First workshop: xx.8/yy (near CERN)

Max Klein HERA-LHeC Manchester 31/1/08 Summary and Proposal endorsed by ECFA As an add-on to the LHC, the LHeC delivers in excess of 1 TeV to the electron-quark cms system. It accesses high parton densities ‘beyond’ what is expected to be the unitarity limit. Its physics is thus fundamental and deserves to be further worked out, also with respect to the findings at the LHC and the final results of the Tevatron and of HERA. First considerations of a ring-ring and a linac-ring accelerator layout lead to an unprecedented combination of energy and luminosity in lepton-hadron physics, exploiting the latest developments in accelerator and detector technology. It is thus decided to hold two workshops (2008 and 2009), under the auspices of ECFA and CERN, with the goal of having a Conceptual Design Report on the accelerator, the experiment and the physics. A Technical Design report will then follow if appropriate.

Max Klein HERA-LHeC Manchester 31/1/08 Quigg The success of HERA and the LHC are the basis for designing a new ep collider. Its physics is unique and it may become reality if we wish so.

Max Klein HERA-LHeC Manchester 31/1/08 More on HERA + LHeC HERA: Talks at EPS07 (Manchester…) U.Klein HERA Summary at DESY Theory Workshop 9/2007 M.Klein and R.Yoshida, Collider Physics at HERA, to appear The H1 and ZEUS Webpages LHeC: J.Dainton et al, JINST 1 (2006) Thanks for the invitation and yesterday’s reminder…

Max Klein HERA-LHeC Manchester 31/1/08 Fundamental questions in lepton-nucleon scattering Is there one form of matter or two, is there substructure of quarks and leptons? Do lepton-quark resonances exist? Do the fundamental interactions unify? What is the dynamics of quark-gluon interactions which is the origin of visible mass? What is the quark-gluon structure of the nucleon? How are quarks confined? Is the Pomeron (really) related to the graviton?? Quarks and gluons in hadronic matter? DIS is the cleanest, high resolution microscope in the world. Thus, DIS over decades has been a cornerstone of HEP.