11 Primakoff Experiments with EIC A. Gasparian NC A&T State University, Greensboro, NC For the...
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Transcript of 11 Primakoff Experiments with EIC A. Gasparian NC A&T State University, Greensboro, NC For the...
11
Primakoff Experiments with EIC
A. GasparianNC A&T State University, Greensboro, NC
For the PrimEx Collaboration
Outline
Physics motivation: The first experiment at JLab: 0 lifetime
Development of precision technique Results for 0 lifetime
Experiments with EIC Summary
2
chiral limit: is the limit of vanishing quark masses mq→ 0.
QCD Lagrangian with quark masses set to zero:
s
d
u
q
GgD
GGqiDqqiDqL
LR
s
RRLLoQCD
)1(2
1
2/
4
1
5,
)(
Large global symmetry group:Large global symmetry group:
)1()1()3()3( BARL UUSUSU
The QCD LagrangianThe QCD Lagrangian
3
Fate of QCD SymmetriesFate of QCD Symmetries
4
• Chiral SUL(3)XSUR(3) spontaneously broken Goldstone mesons π0, η8
• Chiral anomalies Mass of η0 P→γγ ( P: π0, η, η׳)
• Quark flavor SU(3) breaking
The mixing of π0, η and η׳
The The 00, , ηη and and ηη’ system provides a rich ’ system provides a rich laboratory to study the symmetry structure of laboratory to study the symmetry structure of
QCD at low energyQCD at low energy..
Lightest Pseudoscalar MesomsLightest Pseudoscalar Mesoms
55
The PrimEx Experimental ProjectThe PrimEx Experimental Project
Experimental program Precision measurements of:
Two-Photon Decay Widths: Γ(0→), Γ(→), Γ(’→)
Transition Form Factors at low Q2 (0.001-0.5 GeV2/c2): F(*→ 0), F(* →), F(* →)
Test of Chiral Symmetry and Anomalies via the Primakoff Effect
66
Physics Outcome
Fundamental input to Physics:
precision test of chiral anomaly predictions determination of quark mass ratio -’ mixing angle 0, and ’ interaction electromagnetic radii is the ’ an approximate Goldstone boson?
7
First experiment: 0 decay width
eVF
mNc 725.7576 23
3220
0→ decay proceeds primarily via the chiral anomaly in QCD. The chiral anomaly prediction is exact for massless quarks:
Corrections to the chiral anomaly prediction: (u-d quark masses and mass differences)
Calculations in NLO ChPT:(J. Goity, at al. Phys. Rev. D66:076014, 2002)Γ(0) = 8.10eV ± 1.0%
~4% higher than LO, uncertainty: less than 1%
Precision measurements of (0→) at the percent level will provide a stringent test of a fundamental prediction of QCD.
0→
Recent calculations in QCD sum rule: (B.L. Ioffe, et al. Phys. Lett. B647, p. 389, 2007)
Γ() is only input parameter 0- mixing includedΓ(0) = 7.93eV ± 1.5%
8
Decay Length Measurements (Direct Method)
1x10-16 sec too small to measure
solution: Create energetic 0 ‘s,
L = vE/m
But, for E= 1000 GeV, Lmean 100 μm very challenging experiment
Measure 0 decay length
1984 CERN experiment: P=450 GeV proton beamTwo variable separation (5-250m) foilsResult:(0) = 7.34eV3.1% (total)
Major limitations of method unknown P0 spectrum needs higher energies for improvement
0→
9
e+e- Collider Experiment
e+e-e+e-**e+e-0e+e-
e+, e- scattered at small angles (not detected)
only detected
DORIS II @ DESY
Results: Γ(0) = 7.7 ± 0.5 ± 0.5 eV ( ± 10.0%)
Not included in PDG average
Major limitations of method knowledge of luminosity unknown q2 for **
0→
1010
Primakoff Method
22
..4
43
3
2Pr
3
sin)(8
QFQ
E
m
Z
d
dme
ρ,ω
Challenge: Extract the Primakoff amplitude
from the experimental cross section
12C target
Primakoff Nucl. Coherent
Interference Nucl. Incoh.
)log(
2
2Pr
4Pr
2
2
Pr
EZd
Ed
dE
m
peak
peak
11
Previous Primakoff Experiments
DESY (1970) bremsstrahlung beam,
E=1.5 and 2.5 GeVTargets C, Zn, Al, Pb Result: (0)=(11.71.2) eV
10.%
Cornell (1974) bremsstrahlung beam
E=4 and 6 GeV targets: Be, Al, Cu, Ag, U Result: (0)=(7.920.42) eV
5.3%
All previous experiments used: Untagged bremsstrahlung beam Conventional Pb-glass calorimetry
12
PrimEx Experiment at Hall B JLab
JLab Hall B high resolution, high intensity photon tagging facility
New pair spectrometer for photon flux control at high intensities New high resolution hybrid multi-channel calorimeter (HYCAL)
Requirements of Setup: high angular resolution (~0.5 mrad)
high resolutions in calorimeter small beam spot size (‹1mm)
Background: tagging system needed
Particle ID for (-charged part.) veto detectors needed
1313
Fit to Extract Γ(0) Decay Width Theoretical angular distributions smeared with experimental
resolutions are fit to the data
12
C 208Pb
14L. Gan APS, April 15, 2008 14
Estimated Systematic Errors
Contributions Errors
Photon flux 1.0%
Target number 0.1%
Background subtraction 0.9%
Event selection 0.5%
HYCAL response function 0.5%
Beam parameters 0.4%
Acceptance 0.3%
Model errors (theory) 0.25%
Physics background 0.24%
Branching ratio (PDG) 0.03%
Total 1.6%
1515
Current PrimEx Result
() = 7.93eV2.3%1.6%
16
Next Run
16
1717
PrimEx @ High Energies with EICPrimEx @ High Energies with EIC
Experimental program
Precision measurements of:
Transition Form Factors at low Q2 (0.001-0.5 GeV2/c2):
F(*→ 0), F(* →), F(* →)
1818
Primakoff Method
22
..4
43
3
2Pr
3
sin)(8
QFQ
E
m
Z
d
dme
ρ,ω
Challenge: Extract the Primakoff amplitude
12C target
Primakoff
Nucl. Coherent
Interference
Nucl. Incoh.
19
)log( 2
Pr4Pr EZdE
d
d
peak
Increase Primakoff cross section:
Better separation of Primakoff reaction from nuclear processes:
Momentum transfer to the nuclei becomes less reduce the incoherent background
3/12
2
Pr
2
2 AEE
mNCpeak
Why do we need high energy?
20
Direct measurements of slopes:
F(*→ 0), F(* →), F(* →)
Interaction radii:
Fγγ*P(Q2) ≈ 1 - 1/6▪<r2>PQ2
ChPT for large Nc predicts relation between the slopes.
Extraction of Ο(p6) low-energy constant in the chiral Lagrangian
Extraction of decay widths:
Γ(0→), Γ(→), Γ(’→)
Precision test of chiral anomaly predictions
Transition Form Factors at Law Q2
21
Experimental Status for Experimental Status for F(*→ 0)
F(*→ 0) ≈ 1 – a Q2/m2
22
Experimental Status for Experimental Status for F(* →)
2323
PrimEx @ High Energies with EIC Precision Measurement of → decay width
All decay widths are calculated from decay width and experimental Branching Ratios (B.R.):
ΓΓ((η→η→ decay) = decay) = ΓΓ((→→) × B.R.) × B.R.
Any improvement in ΓΓ((→→))
will change the whole will change the whole - sector in PDB- sector in PDB
24
)(2
1ˆ ,
22
222
duud
s mmmmm
mmQ
..)()3( RB
There are two ways to determine the quark mass ratio:
•Γ(η→3π) is the best observable for determining the quark mass ratio, which is obtained from Γ(η→γγ) and known branching ratios:
•The quark mass ratio can also be given by a ratio of The quark mass ratio can also be given by a ratio of meson masses: meson masses:
)(1)(
222
22
2
22 m
mm
mm
m
mQ
QCDKK
kk
o
Determination of quark mass ratioDetermination of quark mass ratio
2525
Corr. )( ..0 meKKmm
)(2
1ˆ re whe,
22
222
duud
s mmmmm
mmQ
ΓΓ((ηη→→33)=)=ΓΓ((→→))××B.B.R.R.
Determination of quark mass ratioDetermination of quark mass ratio
26
• Mixing corrections:
)(cos)(sin
)(sin)(cos00
0
008
008
• DecayDecay constant corrections:
000
888
000
888
cos ,sin
sin ,cos
ffff
ffff
Γ(η/η´→γγ) widths are crucial inputs for obtaining fundamental mixing parameters.
Mixing Angles Mixing Angles
2727
Summary
Extrapolation to Q2=0 will define the radiative decay widths: Γ(0→), Γ(→), Γ(’→)
It looks possible to perform high precision transition form factor measurements of light pseudoscalar mesons at low Q2 with EIC at high energies
Fundamental input to Physics:
precision test of chiral anomaly predictions 0, and ’ interaction electromagnetic radii
extraction of Ο(p6) low-energy constant in the chiral Lagrangian
determination of quark mass ratio -’ mixing angle is the ’ an approximate Goldstone boson?
28A. Gasparian Hall D, March 7, 2008 28
The End
2929
The Primakoff Effect
22
..4
43
3
2Pr
3
sin)(8
QFQ
E
m
Z
d
dme
ρ, ω
Challenge: Extract the Primakoff amplitude
3030
(0→) World Data
0 is lightest quark-antiquark hadron
The lifetime:
= B.R.( 0 →γγ)/(0 →γγ) 0.8 x 10-16 second
Branching ratio: B.R. ( 0→γγ)= (98.8±0.032)% 0
→
±1%
3131
Estimated Systematic Errors
Contributions Errors
Photon flux 1.0%
Target number 0.1%
Background subtraction 0.9%
Event selection 0.5%
HYCAL response function 0.5%
Beam parameters 0.4%
Acceptance 0.3%
Model errors (theory) 0.25%
Physics background 0.24%
Branching ratio (PDG) 0.03%
Total 1.6%
32
Electromagnetic Calorimeter: HYCAL Energy resolution Position resolution Good photon detection efficiency @ 0.1 – 5 GeV; Large geometrical acceptance
PbWO4 crystals resolutionPb-glass budget
HYCALonly
Kinematicalconstraint
33
15 Days
Beam Time and Statistics
Target: L=20 cm, LHe4 NHe = 4x1023 atoms/cm2 Nγ = 1x107 photon/sec (10-11.5 GeV part)<Δσ(prim.)> = 1.6x10-5 mb
N() = NHexNγx<Δσ>xεx(BR)
= 4x1023x 1x107x 1.6x10-32x0.7x0.4 = 64 events/hour = 1500 events/day = 45,000 events/30 days
Will provide sub-percent systematic error