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Arthur M' Moraes

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cone jet finder: sNSD ~ 65 - 73mb. stot ~ 102 - 118 mb (PYTHIA) (PHOJET) ... Distance from the source. ? ( ) dose rates in nSv/h for one SCT barrel module ... – PowerPoint PPT presentation

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Title: Arthur M' Moraes


1
Describing minimum bias and the underlying event
at the LHC with ATLAS
  • Arthur M. Moraes
  • University of Sheffield
  • HEP - ATLAS

University of Glasgow
Glasgow, 20th February 2004
2
Outline
  • Describing minimum bias and the underlying
    event.
  • Comparison of different PYTHIA tunings.
  • PYTHIA vs PHOJET.
  • LHC predictions.
  • Activation levels in the SCT-barrel system
  • Comments and conclusions.

3
Introduction
p
  • What do we expect from a proton-proton collision
    at a centre-of-mass energy of 14 TeV?

?
p
  • There will be a combination of soft (most of
    the time) and hard (occasionally) interactions.
  • Perturbative QCD is highly successful when
    applied to hard processes (large-pt) but cannot
    be applied to soft interactions (low-pt).

  • Alternative approaches to describe soft processes
    are therefore required.

4
Underlying event in charged jet evolution (CDF
style analysis)
Minimum bias events
  • Experimental definition depends on the
    experiment
  • trigger!
  • Minimum bias is usually associated to
  • non-single-diffractive events (NSD),
  • e.g. ISR, UA5, E735, CDF,
  • It is not only minimum bias event!
  • The underlying event is everything except the
    two outgoing hard scattered jets.
  • In a hard scattering process, the underlying
    event has a hard component (initial final-state
    radiation and particles from the outgoing hard
    scattered partons) and a soft component
    (beam-beam remnants).
  • CDF analysis
  • charged particles
  • ptgt0.5 GeV and ?lt1
  • cone jet finder

Df f - fljet
stot 102 - 118 mb
sNSD 65 - 73mb
(PYTHIA)
(PHOJET)
(PYTHIA)
(PHOJET)
5
Model for hadron-hadron collisions (Pythia)
  • Defines two interaction regions in pt scale hard
    and soft processes.
  • Uses perturbative QCD to describe high-pt
    parton-parton scattering.
  • Attempts to extend perturbative (high-pt) picture
    down to low-pt region.
  • Considers the possibility that multiple parton
    scattering takes place in hadron-hadron
    collisions.


n sint
?pt0 ?n (and vice-versa)
pt0
  • Different options for hadronic matter
    distributions.

?d ?probability of hard-scattering (and
vice-versa)
d
6
(No Transcript)
7
F(z) ltnchg gt P(nchg)
z nchg /ltnchg gt
High-multiplicity events are described
differently by each tuning
8
Comments
Transverse lt Nchg gt
  • ATLAS TDR it hasnt been tuned to UE data
    doesnt include double diffraction for
  • minimum bias events uses a model with a small
    hadronic core size doesnt correct for particle
    decays which affect minimum bias distributions
    and doesnt include
  • a pTmin energy dependence.
  • CDF tuning it has been tuned particularly to UE
    data doesnt correct for particle decays which
    affect minimum bias distributions.

Ratio (MC/Data)
Pt (leading jet in GeV)
9
PHOJET
  • Developed mainly for soft and semi-hard particle
    production.
  • Implements ideas of Dual Parton Model for low-pT
    processes.
  • Multiple Pomeron exchanges (sea-quark
    multi-chains) enhances the event activity.
  • Limited to production mechanisms of strong
    interactions.
  • However, useful tool for MB and UE studies where
    jets are involved.

10
PYTHIA vs PHOJET
F(z) ltnchg gt P(nchg)
z nchg /ltnchg gt
11
PYTHIA vs PHOJET
dNchg/d? at ?0
Transverse lt Nchg gt
LHC
Pt (leading jet in GeV)
vs (GeV)
  • PYTHIA models favour ln2(s)
  • PHOJET suggests a ln(s) dependence.

12
Combined ?2 (not the minimum ?2 !)
Multiplicity information nch, dN/d?, KNO
Transverse region (UE) nch and pTsum
  • PHOJET1.12 and PYTHIA6.214 tuned give the best
    global agreement to the data!

13
LHC predictions pp collisions at vs 14 TeV
14
Comments
ATLAS DC
  • PYTHIA6.214 tuned is going to be used for
    ATLAS DC2 production. It is also being used as
    a reference by CMS and ALICE Collaborations.
  • Minimum bias DC samples will be used to validate
    ATLAS Software.
  • Reconstructed minimum bias DC data-samples will
    also be used to develop strategies aimed at
    measuring minimum bias events during the ATLAS
    Commissioning Stage.

Model Improvements GRID resources
  • Model improvements are being investigated in
    collaboration with T. Sjöstrand (PYTHIA6.3 new
    MPI model) and R. Field (CDF run II data).
  • GridPP resources are already being used to
    generate minimum bias and underlying event
    samples.

15
VBF Signal (H?WW?l?l?)
The Underlying Event at the LHC
Prospects for the search for a standard model
Higgs boson in ATLAS using VBF, S.Asai et al,
SN-ATLAS-2003-024 -gt EPJ
  • forward tagging jets
  • correlated leptons
  • low hadronic activity in central region
  • central Higgs production

D. Gaussian PYTHIA6.214 tuned Default PYTHIA6.2
Pythia6.214
e-µ channel only! (MH 160 GeV)
16
Activation of SCT barrel-modules at ATLAS
  • The harsh radiation environment at ATLAS will
    cause the radioactivation of detector components.
  • There can be severe implications for any access
    or maintenance operations
  • Our predictions are based on both calculations
    and measurements.
  • Consider the effects from both neutron capture
    and spallation induced activation.

17
Estimating activity levels
irradiation (180d) and cooling times.
Produced radionuclides per pp event per module
Average number of pp events/s (4 x 108 s-1)
  • 64Cu, 198Au and 110mAg are the dominant
    radionuclides from (n,?).
  • Notice that 1 week after shut down, 110mAg will
    dominate!
  • Concerning spallation induced activation 3H, 7B,
    22Na and 24Na are the dominant radionuclides.
    22Na will be the most important for dose analysis!

18
? and ß dose estimates
? (ß) dose rates in nSv/h for one SCT barrel
module (10 years irradiating)
  • Our estimates indicate that individual
    SCT-barrel modules will fall into the
    slightly-radioactive category.

Maximum ? (ß) dose µSv/h (10 years irradiating)
  • Dose rates from the SCT-barrel will be small
    when compared to other elements of the ATLAS
    experiment. It should not create any serious
    problems.

19
Conclusions and Outlook
  • Current minimum bias and underlying event data
    can be described with appropriate tunings for
    PYTHIA and PHOJET.
  • Multiple parton interactions give a natural way
    of explaining the event activity for both minimum
    bias and the underlying event.
  • We have successfully tuned PYTHIA to both
    minimum bias and the underlying event
    distributions. The tuned model is now being used
    to generate LHC predictions.
  • Our investigations on soft interactions can be
    extended to applications beyond the LHC
    experiment (Tevatron, HERA, ).
  • The levels of radioactivation of SCT-barrel
    modules should not pose any serious problems
    after operation in high radiation environments.
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