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Elastic

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Main part of D experimental analysis: ... primed layers offset from unprimed - read out by PMTs. 6th April 2003. T.Edwards APS Meeting ... – PowerPoint PPT presentation

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Title: Elastic


1
Elastic Diffractive Scatteringat the DØ
Experiment
  • Tamsin Edwards
  • University of Manchester, UK
  • APS Meeting5th - 8th April 2003

2
Hadron scattering at the Tevatron
The Tevatron accelerator collides protons and
antiprotons at a centre-of-mass energy of vs
1.96 TeV at an average rate of 1.7 MHz
  • 60 of total pp cross-section is Inelastic
    Scattering
  • p and p break up
  • Main part of DØ experimental analysis
  • rare hard scale processes production of jets,
    W/Z bosons, b top quarks etc

3
Elastic Scattering
Elastic scattering events
  • p and p scatter with no momentum loss
  • beam particles remain intact, scattered at very
    small angle
  • no other particles produced

What could be passed between p and pthat
transfers momentum without either breaking up?
Exchanged object must have certain properties
  • no charge
  • no colour (colour-singlet)

quantum numbers of the vacuum
Dominantly exchanged object at high energies
given the name Pomeron
  • structure not well understood

4
Elastic Scattering
  • Colour-singlet exchange
  • gives rise to absence of particles or energy
    above threshold in some region of rapidity a
    Rapidity Gap
  • rapidity pseudorapidity ? - ln tan (?/2)
  • where ? is angle of particle with respect to
    beam

The experimental view of the Pomeron is the
thing that causes rapidity gaps
Elastic scattering event
5
Diffractive Scattering
  • Diffractive Scattering takes some momentum

Single Diffractive Scattering
Double Pomeron Exchange
  • To use perturbative predictions, look at hard
    diffractive processes
  • jets, heavy particles also produced

6
Rapidity Gaps
  • Finding rapidity gaps
  • Calorimeter
  • liquid-argon/uranium
  • Luminosity Monitors (LM)
  • scintillators close to beam pipe

Triggers for gap events
  • single gap triggers
  • 1 jet with pT gt 25 GeV
  • gap south no hits in south LM
  • gap north no hits in north LM
  • double gap trigger
  • 1 jet with pT gt 25 GeV
  • no hits in either LM

Analysing rapidity gaps
Look at energy in forward region of calorimeter
  • how much energy is deposited close to beam pipe
    on the gap side?
  • on the non-gap side?

7
Energy in forward calorimeter
Sum of energy of cells above threshold (100MeV)
in first four layers of calorimeter
(electromagnetic) in forward/backward regions
South 2.6 lt ? lt 4.1
North - 4.1 lt ? lt -2.6
North
South
Gap North events
EM Energy (Gev)
EM Energy (Gev)
Shows expected diffractive behaviour peak at
very low energy on gap side
8
The Forward Proton Detector
  • FPD measures track of scattered p or p in
    magnetic field to determine momentum and
    scattering angle

D - Dipole magnet, bends beam around ring Q -
Quadrupole magnets, focus beam S - Separators,
bring beams together to collide
Antiproton Quadrupolespectrometers
Proton Quadrupolespectrometers
Dipolespectrometer
9
The Forward Proton Detector
  • Each spectrometer consists of 2 Roman Pots,
  • vessels containing scintillating fiber tracking
    detector

Proton Up quadrupolespectrometer
Detector
  • U, U diagonal wires
  • X, X horizontal wires
  • trigger scintillator
  • V, V opposite diagonal wires

- primed layers offset from unprimed - read out
by PMTs
10
The Forward Proton Detector
With momentum measurement we can obtain
  • Momentum fraction taken by the pomeron, ?
  • elastic ? 0
  • pomeron exchange dominates for ? lt 0.05

where pi(f) inital (final)momentum
  • Four-momentum transfer, t
  • t ?2, where ? is scattering angle

Much more information is available with FPD than
with gap analysis alone
Acceptance
  • Dipole requires sufficient momentum loss for
    proton to be bent into detector

all t
? gt 0.04
  • Quadrupole requires sufficient scattering angle

t gt 0.8 GeV2
all ?
11
FPD Preliminary Results
Preliminary plots
? and t for elastic scattering events
Expected elastic behaviour
  • ? 0
  • exponential t distribution

?
t (GeV2)
12
Summary
  • Many types of interesting events hard double
    pomeron exchange, diffractive production of
    jets, W/Z bosons, heavy quarks...
  • previous papers from UA8, Hera, DØ Run I have
    driven current experimental interest
  • Gap analysis can already tell us a lot about
    these events
  • Forward Proton Detector will tell us even more
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