Diffraction at LHC, Tevatron and HERA

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Presentation transcript:

Diffraction at LHC, Tevatron and HERA HCP 2004, Michigan State University, June 14th - 18th 2004 Brian Cox Diffraction at LHC, Tevatron and HERA Even ‘normal’ people are becoming interested in diffraction at the LHC … Improved mass resolution Only 0++ (or 2++) systems produced bb background strongly suppressed Very schematically, it’s a glue-glue collider where you know the beam energy of the gluons Is ‘Central Exclusive Double Pomeron’ process a useful tool at LHC? Do we understand diffractive processes well enough to use them for searches?

The Diffractive Program at the LHC FORWARD PHYSICS Each RP station consists of two Roman Pot Units separated by 3.4 m, centered at 240.0 m from IP1 TOTEM Design!

Atlas has alternative very high b Atlas has alternative very high b* (2625m) optics to get to coulomb region 0.00056 < |t| < 0.030 GeV2

The Experimental Challenges for Exclusive States M2 = x1 x2 S Where x1,2 are the fractional momentum losses of the outgoing protons horizontal offset = Dx To get  ~ 0.005 proton (M ~ 70 GeV) 2.5mm from beam (10s) pots must be > 250 m from IP -> cold region, & level 1 trigger not possible K. Österberg 420 m 308 m 215 m

Particularly promising scenarios for CEDP If the coupling of the Higgs-like object to gluons is large, double proton tagging becomes very attractive ‘Difficult’ regions of the MSSM The MSSM with explicit CP violation (CPX)

An example : The intense coupling regime of the MSSM e.g. mA = 130 GeV, tan b = 50 (difficult for conventional detection, but exclusive diffractive favourable) L = 30 fb-1, DM = 1 GeV S B mh = 124.4 GeV 71 3 events mH = 135.5 GeV 124 2 mA = 130 GeV 1 2 Alan Martin Manchester Dec 2003 The intense coupling regime is where the masses of the 3 neutral Higgs bosons are close to each other and tan b is large suppressed enhanced 0++ selection rule suppresses A production: CEDP ‘filters out’ pseudoscalar production, leaving pure H sample for study Kaidalov, Khoze, Martin, Ryskin hep-ph/0311023

The MSSM with explicit CP violation - the ‘CPX’ scenario Imagine a light scalar which couples predominantly to glue, and decays to b jets … would we see it at LEP, Tevatron or LHC? “there are small regions of parameter space in which none of the neutral Higgs bosons can be detected at the Tevatron and the LHC” Medium grey Dark grey In the CPX scenario, the three neutral MSSM Higgs bosons, (CP even) h0 and H 0, and (CP odd) a mix to produce 3 physical mass eigenstates H 1 , H 2 and H 3 with mixed CP M. Carena, J. Ellis, S. Mrenna, A. Pilaftsis and C. E. M. Wagner, Nucl. Phys B659 (2003) 145

CPX MSSM Higgs b bbar very difficult because of large background: QCD Background ~ 0++ Selection rule Also, since resolution of taggers > Higgs width: s in fb But tt mode has only QED background CP even CP odd active at non-zero t Direct evidence for CP violation in Higgs sector B.C., Forshaw, Lee, Monk and Pilaftsis hep-ph/0303206 Khoze, Martin and Ryskin hep-ph/0401078

Do we understand diffraction well enough to use it as a search tool? Important background to exclusive process As with all processes at hadron colliders, the structure functions are of prime importance

Diffractive Structure Functions at HERA

Factorisation does not hold in PP An unproved statement : If there are no multi-parton interactions, then the diffractive structure functions measured at the Tevatron are ~ the same as those at HERA

Factorisation in PP R(SD/ND) R(DPE/SD) K. Goulianos Jeff Forshaw HERA - LHC workshop R(SD/ND) R(DPE/SD) M. Klasen HERA - LHC Workshop K. Goulianos

How reliable are the predictions? The cross section ~ factorises … Hard subprocess cross section Effective luminosity for production of mass M at rapidity y … so can be checked by measuring higher rate processes at Tevatron and LHC

How reliable are the predictions? Q2 Q3 Q4 A1 A2 P1U P2I P2O P1D D2 D1 23 33 59 57 Veto

Summary and work in progress Real discovery potential in certain scenarios Possibility to measure Higgs branching ratio to e.g. b or t - complementary information to conventional searches Azimuthal asymmetries allow direct measurement of CP violation in Higgs sector Assuming CP conservation, any object seen with 2 tagged protons has positive C parity, is (most probably) 0+, and is a colour singlet Need theoretical and experimental verification of the cross section and background predictions If we can get the pots close enough for level 1 trigger, and increase the acceptance at 120 GeV, this project is extremely exciting - can we do it? http://glodwick.hep.man.ac.uk/conference

Jeff Forshaw