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Title: A precision measurement of the neutral pion life time: new results from the PrimEx experiment


1
A precision measurement of the neutral pion life
time new results from the PrimEx experiment
International Conference New Trends in High
Energy Physics Yalta, Crimea, Ukraine September
15 - 22, 2007 I. Larin, ITEP, Moscow on behalf
of the PrimEx collaboration
2
Participating Institutions
  • a Arizona State University, Tempe, AZ b
    Catholic University of America, Washington, DC
    c Chinese Institute of Atomic Energy, Beijing,
    China d Eastern Kentucky University, Richmond,
    KY e George Washington University, Washington,
    DC f Hampton University, Hampton, VA g
    Institute for High Energy Physics, Chinese
    Academy of Sciences, Beijing, China h Institute
    for High Energy Physics, Protvino, Moscow region,
    Russia i Institute for Theoretical and
    Experimental Physics, Moscow, Russia j Kharkiv
    Institute of Physics and Technology, Kharkiv,
    Ukraine k Massachusetts Institute of
    Technology, Cambridge, MA l Norfolk State
    University, Norfolk, VA m North Carolina AT
    State University, Greensboro, NC n North
    Carolina Central University, Durham, NC o
    Southern University at New Orleans, New Orleans,
    LA p Thomas Jefferson National Accelerator
    Facility, Newport News, VA q Tomsk
    Polytechnical University, Tomsk, Russia r
    University of Illinois, Urbana, IL s
    University of Kentucky, Lexington, KY t
    University of Massachusetts, Amherst, MA u
    University of North Carolina at Wilmington,
    Wilmington, NC v University of Texas at El
    Paso, El Paso, TX w University of Virginia,
    Charlottesville, VA x Yerevan Physics
    Institute, Yerevan, Armenia

3
Physics Motivation
  • p0 radiation width is one of the most precise
    fundamental predictions of the low energy QCD.
    Number of quark color states is a parameter of
    the calculations
  • For massless quarks, width is given by the
    formula
  • G(p0 gg) a3Nc2mp3 / 576p3Fp2 7.725 eV (Nc
    3)
  • More precise calculations are giving
  • 7.93eV 1.5 (QCD sum rules, B.L.Ioffe and
    A.G.Oganesian hep-ph/0701077 )
  • 8.10eV 1.0 (Chiral theory, J.L.Goity et al
    Phys Rev D66 076014 / 2002)
  • Which precision can be achieved in experimental
    measurements?

4
Existing Measurements of p0 Meson Decay Width
Experimental measurements of the radiative width
give 7.84eV 0.56eV. It is 7 error, could it
be reduced, we can check QCD predictions with the
precision close to the theory uncertainties. It
is the challenge for the PrimEx experiment!
5
The Primakoff Effect
The PrimEx experiment has utilized the Primakoff
effect to measure p0 radiative width
  • p0 photoproduction in coulomb field of nucleus
  • Equivalence of photoproduction (gg p0) and
    radiative decay (p0 gg) gives raise to linear
    dependence between cross section of primakoff
    production radiative width
  • p0 production for this mechanism goes at very
    small (few MeV) momentum transferred
    (corresponding production angles are fractions of
    milliradian for the PrimEx conditions)

6
Thomas Jefferson National Accelerator Facility
(TJNAF)
  • PrimEx physics data have been collected during
    the 2004 fall run in TJNAF Hall B
  • Narrow monochromatic electron beam, injected from
    FEL
  • Energy of electron beam for PrimEx run was 5.75
    GeV
  • The PrimEx experiment has utilized tagged photon
    beam with well known energy (in the range of
    4.95.5 GeV) formed from the electron beam

7
PrimEx Setup
  • For high precision
  • JLab Hall B high resolution high intensity
    photon tagging facility (tight photon energy and
    flux control)
  • New state of art high resolution hybrid
    multi-channel calorimeter HYCAL (measure po
    angular distribution well to separate various
    amplitudes )
  • New pair spectrometer for photon flux control
    at high intensities
  • Variety of targets to test validity of
    background extraction (sPrimakoff a Z 2)
  • Ability to measure QED processes (Compton and
    pair production) to validate setup and analysis
    techniques

Distance from target to calorimeter 7.3?
8
Hall-B Photon Tagger
  • Serves as a high precision photon flux meter
  • Photon beam energy resolution - 0.1
  • Tagging signal time resolution - 0.10.2 nsec

9
PrimEx Targets Used For p0 Run
Carbon target pyrolitic graphite with thickness
of 5 X0 or 9.6mm and density of 2.2 g/cm3
Thickness tolerance - 0.1
Lead target monoisotopical lead-208 spinless
nucleus, foil with the thickness of 5 X0 or
0.3mm Thickness tolerance - 0.3
10
ee- pair spectrometer
plastic scintillators
Pair spectrometer serves as an online relative
flux monitor detecting ee- pairs from the
target. Needs to ensure high precision of the
beam flux measurements
dipole magnet
11
PrimEx Hybrid Calorimeter HyCal
  • Transverse size 1.2m x 1.2m
  • thermostated at 14?
  • Central part
  • 1152 PbWO4 modules (scintillators)
  • Peripheral part
  • 576 lead glass modules (Cherenkov counters)

12
PbWO4 Crystals
  • Scintillators
  • Size 20.5 x 20.5 x 180.0 mm3
  • Transverse size and its tolerance
  • Specified 20.5 0.0 -0.1mm
  • Measured 20.47 0.02mm
  • Density 8.3 ?/cm3
  • Radiation length 0.89 cm
  • Light emission time (fast component) 15 5 ns
  • Refraction index 2.2
  • Light yield 80 Photons/MeV

13
HyCal Calibration
  • HyCal calibration has been performed during
    snake scans with HyCal placed on transporter
    and exposed to tagged beam
  • Additionally physical calibration with p0s has
    been performed using all collected p0s

14
HyCal Resolution
  • PWO part of HyCal (5GeV ?)
  • 1ns time signal resolution (used for triggering)
  • 2.3MeV ? mass resolution
  • 0.02 ? production angle resolution
  • 1.7 and 0.9 ? energy resolution (w/o and with
    ? mass constraint)
  • Lead glass Cherenkov modules
  • approximately twice worse resolution values

15
PrimEx Production Run
  • PrimEx data have been collected during
    October-November 2004
  • p0 production runs (with full magnetic field in
    PS-magnet). Working energy range 4.95.5GeV
    (first 11 T-counters).
  • ee- production runs (intermediate magnetic field
    in PS allowed pairs to hit calorimeter)
  • Compton runs (zero field in PS-magnet allows
    compton pairs to reach HyCal)

16
Typical p0 event (real data) on the HyCal event
display
17
p0 Reconstruction2? invariant mass spectrum
Crystal part of HyCal
Elastic p0s, Beam energy (well known from Tagger)
has been used to correct cluster energies
(Resolution dominated by coordinate
reconstruction).
Elastic and inelastic p0s, using energies
reconstructed by HyCal
18
?0 elasticity spectrum(for PWO part of HyCal)
p0 elasticity E(?) E(p0)
Elastic yield was extracted using fitting
procedure and used in further analysis
s _at_ 0.9
19
?0 production terms
Angular distribution enables separation of
amplitudes
Primakoff term
Strong production Incoherent Coherent
20
Fit to Extract ?0??? Decay Width p0
distribution on production angle (PWO part of
HyCal)
  • p0 production terms
  • Sum of all
  • Coulomb
  • Strong
  • Interference
  • Incoherent

Theoretical distributions of these processes were
smeared with the experimental resolution
21
w and r background for Carbon
p0 distribution on production angle
contribution from r and w was varied with
its cross-section uncertainty (which is
20) Estimated systematic error contribution by
this variation is 0.24
22
PrimEx Preliminary Result
?(????) 7.93eV?2.1?2.0
23
Systematics check Compton process
Radiation corrections were taken into account in
the theoretical calculations since high precision
is needed
24
Systematics check Compton process
Measured Compton cross section at ? beam energy
range 4.95.5GeV is in agreement with the theory
within stat. and syst. errors
25
Systematics check ee- Pair Production
  • Bethe-Heitler
  • Virtual Compton scattering
  • Radiative effects
  • Atomic screening
  • Electron field pair production

Corrections were taken into account in the
theoretical calculations since high precision is
needed
26
Systematics check ee- Pair Production

Measured pair production cross section at ? beam
energy range 4.95.5GeV is in agreement with the
theory within stat. and syst. errors
27
?0 Rad. Width Error Budget (preliminary)
28
PrimEx Future Plans
  • publish 2004 run physics results in the nearest
    future
  • prepare for the new run 2008-2009 to collect an
    extra statistics with the optimized experimental
    conditions (taking into account existing
    experience and therefore with reduced
    systematical error)
  • go to 12GeV beam measurements after upgrade of
    JLab accelerator. Precision measurement of h
    meson radiation width

29
Conclusion
  • Precision measurement of p0 meson rad. width
    gives the possibility to check QCD prediction,
    based on the number of quark color states.
    Required precision of the measurements has pushed
    the serious requirements to the experimental
    setup
  • In 2000-2004 the unique hybrid electromagnetic
    calorimeter (HyCal, which is one of the main
    parts of the PrimEx setup) was assembled at TJNAF
    Hall-B
  • Obtained resolution for p0 mass is 2.3MeV for the
    crystal part of HyCal. Usage of the Photon Tagger
    information about beam energy gives further
    improvement of this value up to 1.3MeV
  • High quality data (12C and 208Pb nuclei at photon
    beam energy 4.95.5GeV) have been collected
    during fall 2004 run
  • Quality of the data is defined by the excellent
    energy and spatial resolutions of the HyCal and
    the precise measurement of the photon beam energy
    and flux with the unique Photon Tagger
  • Measured p0 radiation width (preliminary result)
  • 7.93eV ? 2.1 (stat.) ? 2.0 (syst.)

30
Spare Slides
31
Decay Length Measurements (Direct Method)
An experiment had been done at CERN, in 1984,
P450 GeV proton beam 2 variable (5-250?m)
foils Result ?(?0???) 7.34eV?3.1(total)
Dominant systematic error Uncertainty in P?
(?1.5)
32
Formfactors
  • Distorted formfactors have been calculated with
    most up-to-date charge density distribution
  • (E.Offermann, L.Cardman et al, Phys Rev C 91
    Vol.44)

12C charge density
12C strong formfactor
33
Elastic p0 yield extraction
Method 1 conventional Elasticity and Invariant
mass distributions fitting
Example of elasticity distribution
Example of invariant mass distribution
34
Elastic p0 yield extraction
Method 2 rotation of Elasticity - Invariant mass
2D distribution, hybrid mass analysis
35
Elastic p0 yield extraction
Method 3 Invariant mass with elasticity
constraint analysis
36
w and r decays background
?0 elasticity spectrum E(?0) E(?)
Data, Carbon target
Simulated contribution from w and r
decays, scaled according to known cross-section
values to Photon beam flux from the data
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