QCD@IPPP June 2006 Kaidalov Bashir Ryskin Khoze Pennington Diffraction Papagallo Ball Martin Roberts Stirling Partons Hadrons Zwicky Buckley QCD Twistor Space Khoze Georgiou Glover De Roeck Huston Cross sections Resummation Maxwell Van Acoleyen Vogt Brein Richardson Will discuss in future Monte Carlo Krauss open session Hamilton Grellscheid Figy Signer Stockinger Martin, Stirling + Roberts, Thorne MRST Parton distributions 1.

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Transcript QCD@IPPP June 2006 Kaidalov Bashir Ryskin Khoze Pennington Diffraction Papagallo Ball Martin Roberts Stirling Partons Hadrons Zwicky Buckley QCD Twistor Space Khoze Georgiou Glover De Roeck Huston Cross sections Resummation Maxwell Van Acoleyen Vogt Brein Richardson Will discuss in future Monte Carlo Krauss open session Hamilton Grellscheid Figy Signer Stockinger Martin, Stirling + Roberts, Thorne MRST Parton distributions 1.

QCD@IPPP
June 2006
Kaidalov
Bashir
Ryskin
Khoze
Pennington
Diffraction
Papagallo
Ball
Martin
Roberts
Stirling
Partons
Hadrons
Zwicky
Buckley
QCD
Twistor
Space
Khoze
Georgiou
Glover
De Roeck
Huston
Cross
sections
Resummation
Maxwell
Van Acoleyen
Vogt
Brein
Richardson
Will
discuss
in future
Monte Carlo
Krauss
open session
Hamilton
Grellscheid
Figy
Signer
Stockinger
Martin, Stirling + Roberts, Thorne
MRST Parton distributions
1. Uncertainties on partons I: experimental errors
Uncertainties due to errors on experimental data fitted obtained using
both the Hessian and Lagrange multiplier approaches.
Examples: resulting errors on predictions for W, Higgs prod., and CC
DIS
2. Uncertainties on partons II: theoretical errors
Uncertainties due to NLONNLO, ln(1/x) and ln(1-x) effects,
absorptive corrections, higher twist, choice of input parametrization,
isospin violation….
Martin, Stirling + Roberts, Thorne
MRST Parton distributions
3. Physical gluons and high ET jets
Physical large x parametrization of gluon
--driven by valence quarks in MSbar scheme
--gives excellent description of Tevatron jets
Martin, Stirling + Roberts, Thorne
MRST Parton distributions
4. Parton distributions incorporating QED contributions
Includes aQED contributions: treats photon as a parton.
Automatically includes isospin violationexplains 50% of NuTeV anomaly
Fewer high x up than dn, since more photons emitted from u.
Proton PDFs
Neutron PDFs
Martin, Stirling + Roberts, Thorne
MRST Parton distributions
5. The role of FL(x,Q2) in parton analyses
Motivated by the forthcoming measurements of FL at HERA
-- NNLO analysis gives better description at low x
-- some evidence of higher twist contributions
6. MRST partons generated in a fixed flavour scheme
Needed for existing Monte Carlos and
other calculations in FFNS.
Martin, Stirling + Roberts, Thorne
MRST Parton distributions
Personnel changes
Dick Roberts has retired, and Graeme Watt (UCL) has joined the collab.
Future studies
Complete NNLO analysis including all recent data in VFNS,
and providing quantitative errors on partons
With Misha Ryskin and Graeme Watt (UCL) :
1. Determination of diffractive parton densities applying our novel pQCD
approach to the new diffractive data.
2. Determination of the structure of the pion by extending our analysis of
the HERA leading neutron data.
Ball, Zwicky
From Inclusive to Exclusive Processes
• Parton distributions:
One particle probability amplitudes
• Multiparton Distributions:
Correlations and interference effects
Ball, Zwicky
From Inclusive to Exclusive Processes
Concept: Light-cone distribution amplitudes
Particle wave functions at small
transverse separation b~1/Q:
Partial-wave expansion using conformal symmetry of massless QCD
Analysis of higher twist effects using QCD equations of motion
Applications: EM form factors, photon transition form factors, nonleptonic B decays…
Khoze, Martin, Stirling + de Roeck, Kaidalov, Ryskin
Diffractive processes as a means to study new
physics at the LHC
 the theoretical motivation behind the recent proposals to add
the Forward Proton taggers to the LHC experiments
 the basic ingredients of Durham approach through the eyes
of existing Tevatron and HERA diffractive data
 direct engagement with experimentalists in analysing and
planning the forward measurements, in part., FP420 R&D.
Khoze, Martin, Stirling + de Roeck, Kaidalov, Ryskin
Diffractive processes as a means to study new physics
at the LHC
Main advantages of CED
Higgs production
 Accurate mass measurement
(irrespective of the decay mode).
 Quantum number filter/analyser.
(0++ dominance ;CP-even)
 H ->bb not swamped by
background
 H →WW*/WW () less
challenging experimentally
Theoretical challenges :
 need for developed and well
tested models for soft
diffraction
 unusually & uncomfortably
large higher-order QCD effects
(e.g. Sudakov. and nonSudakov Logs… ).
 no suitable conventional
analytic or MC results readily
available (colour singlet, Jz=0)
Khoze, Martin, Stirling + de Roeck, Kaidalov, Ryskin
Diffractive processes at the tevatron
CDF
Heinemeyer, Khoze, Ryskin, Stirling, Tasevsky, Weiglein
Diffractive processes as a means to study new physics
at the LHC
PRELIMINARY
Khoze, Stirling + de Roeck
The FP420 R+D project
Close ties with Manchester and
other UK FP 420 members.
Successful annual IPPP Manchester Forward workshops
(from 2001)
Joint research and publications.
The LHCC acknowledges the
scientific merit of the FP420 physics
program and the interest in exploring
its feasibility - LHCC
The panel believes that this offers a
unique opportunity to extend the
potential of the LHC and has the
potential to give high scientific return.
- PPARC PPRP
Glover, Anastasiou, Garland, Koukoutsakis, Tejeda-Yeomans,
+ Heinrich, Gehrmann, Gehrmann-De Ridder, Remiddi
NNLO Jets in e+eTwo loop matrix elements computed
some time ago
Antenna subtraction scheme to
isolate infrared divergences
Analytic integration of infrared poles
Analytic cancellation of infrared poles
Numerical implementation now in
progress
Glover + Gehrmann, Gehrmann-De Ridder, Heinrich
NNLO Jets in e+e-
T dσ
σ dT
Other colour factors in progress, expected later this year
Glover, Pires
NNLO Jets in pp
Needed for better determinations of
PDF’s and αs
NLO accuracy at best ±30%
NNLO accuracy ~10%
Using sector decomposition to
extract phase space singularities
Aim to have first results by start of
LHC
Signer + Pineda
Threshold resummation for heavy quarks
 At threshold there are two
small parameters αs and v
 Also several scales m, mv and
mv2
 ln(v) large and must be
resummed
 Complete result at NLL and
including some NNLL terms
Dinsdale, Maxwell
Infrared resummation
 Extended effective charge scheme to
include resummation of infrared
logarithms
 Size of fitted power correction C1/Q
varies with order, but more stable
extraction of ΛMS
ΛMS
C1/Q
Thrust
Pennington, Boglione, Edera, Fischer, Papagallo, Williams + Bashir
Hadrons and confinement
 Hadron spectrum
 Chiral symmetry breaking
 Dynamical mass generation
 Confinement
 Dyson-Schwinger equations
hep-ph/0504262
Pennington, Boglione
γγ
π+ π- and π0 π0
Couplings probe hadron dynamics
peak
Mark II
hep-ph/0504262
dip
Many other activities
Infrared finite amplitudes
LHC MSSM cross sections
Non-perturbative vertices with SDE
Finite volume effects in quenched lattice GT
Isospin effects in D decay
DRED v DREG for SUSY
One-loop multi-leg processes
Higgs cross sections
NNLO splitting functions/coefficient functions
Twistor phenomenology
Signer, Brown
Brein
Pennington, Bashir,
Williams
Pennington, Fischer
Pennington, Edera
Signer, Stockinger
Glover, Badger
Figy
Vogt
Ozeren, Georgiou,
Badger, Khoze,
Glover, Stirling
QCD related PhD Theses
Tejeda-Yeomans (01)
Parton-Parton Scattering at Two-Loops
Kimber (01)
Unintegrated Parton Distributions
Anastasiou (01)
Two-Loop integrals and QCD scattering
Andersen (02)
Monte Carlo Studies of BFKL Physics
Adamson (02)
Vector boson pair production at hadron colliders
Williams (02)
Hadronic Higgs Production with Forward Jets
Koukoutsakis (03)
Higgs Bosons and QCD Jets at Two Loops
Garland (03)
Two-loop helicity amplitudes in QCD
Watt (04)
Parton Distributions
Howe (04)
Infrared Behaviour of QCD Observables
Forde (04)
Infrared Finite Amplitudes
Morley-Fletcher (05)
Covariant infrared finite amplitudes
Dinsdale (05)
The scheme-dependence of power correction fits to event shape
observables
Birthwright (05)
Two loop vertices and tree level multicollinear limits in QCD
http://www.ippp.dur.ac.uk/Research/theses.htm
QCD related workshops
18 workshops/schools including
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





5 x Manchester forward physics workshops
57th SUSSP school on LHC Phenomenology
Light-Cone Physics: Hadrons and Beyond (Swansea)
Multiparticle Production in QCD Jets
Workshop on TeV-Scale Physics (Cambridge)
Monte Carlos at Hadron Colliders
Future Physics at HERA
QCD related PDRA’s
Carlo Oleari, Zoltan Nagy, Elena Boglione, Gudrun Heinrich,
Giulia Zanderighi, Gabriele Travaglini, Peter Marquard,
Dominik Stockinger, Christian Fischer, Karel Van Acoleyen,
Oliver Brein, Terrance Figy, Laura Edera, Fulvia de Fazio, …
…and finally
• Advancing Collider
Physics from Twistors to
Monte Carlos
• Aug 27-Oct 26 2007
Khoze, Martin, Stirling + de Roeck, Kaidalov, Ryskin
Diffractive processes: the next steps
Comprehensive study of the radiative backgrounds to the H->bb CEDP,
application to the Higgs physics at PC@ILC.
Leading neutron spectra at HERA as a way to gauge the absorptive
effects and enhanced Pomeron contributions
Detailed investigation of the BSM Higgs sector in diffractive processes
 Study of the NLL- effects in the mass-suppressed Jz=0 gg/-> qq
amplitudes
Khoze, Martin, Stirling + de Roeck, Kaidalov, Ryskin
Diffractive processes: the mid-term
1. Very Optimistic scenario:
FP-420 is approved, and Higgs is found at the LHC.
work needed to improve the accuracy of calculations to match
experimental precision
2. FP420- unfriendly scenario:
Higgs is found, but FP-420 is not approved or long delayed.
application of the ‘event colour portrait’ technique to disentangle the
Higgs signal from the QCD backgrounds.
3. Pessimistic scenario:
Elementary Higgs is not found and FP-420 is not approved.
Comprehensive soft and semi-soft physics programs for TOTEM,
CMS-TOTEM and ATLAS (possibly ALICE). Photon-induced
interactions at the LHC.