the primex experiment – symmetry breaking in the chiral ... · • the primex experiment at...
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The PRIMEX Experiment: A Fundamental Test of the Chiral
Anomaly Prediction in QCD
Erik Minges
April 23rd, 2010
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Outline• Symmetry and conservation Laws
– Overview and examples
• PRIMEX physics motivation
– The Chiral Anomaly
• Experimental Setup
• PRIMEX first run results
• Prototype detector beamtest
– Energy calibration, shower profile, position resolution
– Conclusion
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Symmetry – What is it?
• Generalized to mean invariance
– A system which remains unchanged under a certain kind of transformation.
• Rotational symmetry of a pencil
Rotational Symmetry
Symmetry Breaking
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Symmetry cont.• Powerful tool in physics
– In 1905, Amalie Noether determined the connection between symmetry and conservation laws
• Noether’s theorem – For every continuous mathematical symmetry, there is a corresponding conservation law.
• “it is only slightly overstating that physics is the study of symmetry.” – Philip Warren Anderson
– American Physicist and Nobel Laureate
• Contributions to theories of localization, antiferromagnetism, and high-temperature superconductivity
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PRIMEX Experiment
• The PRIMEX experiment at Thomas Jefferson National Lab is to measure the lifetime of the π0 particle with high precision. This experiment is a very important test of Quantum Chromodynamics (the theory to describe the strong interaction).
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PRIMEX Physics Motivation
• Prediction of the decay width in ChiralAnomaly is exact in the Chiral limit.
– However quarks have mass.
– Leads to correction in theory.
• Neutral Pion decay measured to test fundamental prediction of low energy QCD.
– High precision measurement of decay rate, dominated by axial anomaly.
0
0
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Chiral Anomaly• Axial symmetry of the Classical Lagrangian of
Quantum Chromodynamics is broken in the Chirallimit.
– Chiral limit is when the up, down quark masses vanish.
• This symmetry breaking is of pure Quantum mechanical origin due to quantization.
• The Lagrangian has continuous symmetry, but no conservation law associated with it
– i.e. - no conserved current
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Confirmation of Quark Color• In the chiral limit, the predicted decay amplitude
– Where is the number of quark colors in QCD and is the Pion decay constant.
• Precise predicted decay width
• Number of quark colors will be directly measured by this experiment
– Number colors most fundamental parameter in Physics
1210513.2)3(
GeVf
NA C
MeVf 42.92
3CN
eV
Am725.7
64
23
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Primakoff Effect
• Virtual photon from nucleus of target interacts with tagged photon from incident photon beam.
– Virtual photon and tagged photon create neutral Pi meson
• Photopion production
from Coulomb field of nucleus.
• Pion decay in forward direction, so
need good central resolution.
– Pi zero has high branching ratio to decay into 2 gamma rays, which HYCAL can detect.
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Experimental Setup
Electron beam passing through
nucleus field and change momentum,
produce Bremsstrahlung radiation
Measure energy and momentum
of scattered electrons yield energy
and momentum of gamma produced
Radiator
Physics target
(Primakoff)
Magnet measure pair production to monitor
photon flux and sweep out charged particles
Helium bag less particle interaction
than air and cheaper than vacuum
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Status of PRIMEX
PrimEx-I
() = 7.82eV2.2%2.1%
Leading Order
Chiral Anomaly
Next toLeading Order
Chiral Anomaly
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Analysis Results for the 6x6PbWO4 Crystal Prototype
Detector Beam Test
Center Crystals PbWO4
Surrounding Lead Glass
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My Project for PRIMEX
• What is the need for an energy calibration?– 36 PbWO4 crystals detect incident beam energy via ADC
– Meaningful average pulse height signal from ADC requires calibration of each crystal using known incident beam energies
• How is the incident beam energy found?– x-y coordinate detector with 60 scintillating fibers on each axis
• Detects position of incident electrons.
• Each fiber approximately 2 mm in diameter
– Dipole magnet’s field yields incident energy of electrons• Incident electron beam energy as a function of X – fiber number is
e
e
36241 1011645.0*1046112.0*1015153.05004.3 XXXXEbeam
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Relative Energy Calibration• Alignment
– Each crystal needs to have the same response
– Align each individual crystal center
• Assume all incident energy is deposited at center of crystal
• Assume no energy is lost due to leakage into surrounding crystals
• Find mean ADC at center of crystal, divide by known incident energy
Ebeam=A*(mean ADC)
i.e. For run 435 (centered on crystal 26)
Ebeam = E(29) = 3.98145729105
(mean ADC) = 5413
... so A = 7.35536171E-04!!!
adc(1) for run 435 cut at (X=29) and (Y=31)
mean ADC = 5413
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Global Energy Calibration• Absolute scale from 5x5 cluster size
• Shower interacts in several crystal– Sum all deposited energy in surrounding crystals to account for leakage
Ebeam = B*[ ∑ Ai * (mean ADC)i ]
419
i.e. For run 419 (centered on crystal 15)
Ebeam = E(29) = 3.98145729105
∑ Ai * (mean ADC)I = 5.095
... so B = .781444021796 !!!
with σ/Ere = .018637880275
Now just take the average value ofthe four center crystals
Bavg = .781858818128
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ResultsError bars for (Ere/Ebeam)associated with run 413
21 22 23
- Ratio of Energies Deposited in a single module
Minimum deposited energy is at boundary of crystal. (As expected)
Maximum deposited energy is at center of crystal.
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Results
21 22 23
Error bars for (σ/Ere)associated with run 413
21 22 23
- Energy Resolution of the Prototype
Energy resolution at center is greater than at boundaries of crystal. (As expected)
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Results - Shower ProfileThe shower profile measures the dependence of the
average pulse-height ratio for different crystal channels
1.) Adjacent Channel ratio
Ai/Ai+1
2.) Adjacent Row ratio
Aj/Aj+1
3.) Separated Channel ratio
Ai+1/Ai-1
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Results - Adjacent Channel Ratio
Run 435 for E26/E27
2726
1
Boundary
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Results - Adjacent Row Ratio Run 422 E3,9,15/E4,10,16
3, 9, 15 4, 10, 16
1
Boundary
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Results - Separated Channels Ratio Run 435 for E28/E26
26 27
Center: 27
28
1
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Reconstructed Position Method
• Center of Gravity Method
Weight factor for cell
• Linear Weight
where,
• Logarithmic Weight
)(
*)(
i
N
i
i
ii
N
i
i
cal
E
xE
x
)( ii E
T
iii
E
EE )(
N
i
iT EE
T
iii
E
EWE ln,0max 0
thi
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Linear - Reconstructed Position
3x3 – run 389 3x3 – run 422
8
9
10
9
10
11
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Linear - Reconstructed Position5x5 – run 413
21
22
S shape indicates some systematic shift from the method incorporated.
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Linear Position Resolution
3x3 – run 389 3x3 – run 422
8 9 10
9 10 11
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Linear Position Resolution5x5 – run 413
21 22Position resolution worst at boundaries and best at center
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Logarithmic Reconstructed Position
3x3 – run 389 3x3 – run 422
8
9
10
9
10
11~ %3 error (leakage)
~ %3 error (leakage)
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Logarithmic Reconstructed Position5x5 – run 413
21
22
(No systematic shift)
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Logarithmic Position Resolution
3x3 – run 389 3x3 – run 422
8 9 10 9 10 11
3% error
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Logarithmic Position Resolution5x5 – run 413
21 22
1% error
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Linear or Logarithmic Weight?
• Linear weight - large systematic errors
• Radial energy fall off of showers is exponential
• Energy deposited in the module decreases exponentially as a function of the distance from the point of incidence.
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Logarithmic Weight
• Ideal weight must employ a logarithmically weighted energy due to the exponential fall off of the shower profile
• The logarithmically weighting of the deposited energy signals produce the best results
• Which is what we were expecting from the results
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Conclusion
• PRIMEX Experiment provide precision test on Chiral Anomaly prediction.
• Energy Resolution
– %1.7 at the center and %2.2 at boundaries
– Worse at edge of crystals
– Due to fluctuation of shower and energy leakage
• Reconstructed Position
– Center of gravity
• Linear has large systematic error
• Logarithmic is almost linear; small systematic shift
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Thank You PrimEx!… and my mentor: Dr. Gan - UNCW
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Conservation Laws
• Symmetries in nature lead to conservation laws
– A particular measurable property of an isolated physical system does not change as the system evolves
– Corresponds to a conserved physical quantity.
• Conservation of energy, linear momentum, angular momentum, electric charge, probability, mass, etc.
• Usually derived from Lagrangian dynamics
– A reformulation of classical mechanics that combines conservation of momentum with conservation of energy.
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Lagrangian Dynamics
• Lagrangian of a system is a classical method to derive Newton’s second law of motion, .
• Forces are hard to find.
– Lagrangian utilizes conservation of energy
• , where is a generalized coordinate system
• Lagrangian equation of motion:
– Conservation Law
• If , where C is a constant.
amF
0
ii x
L
dt
d
x
L
Cx
L
x
L
ii
0
ix txUtxxTxxL iiiii ,,,,
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Conservation Law second example
• Parity Violation
– Flip either one, or all spatial variable signs.
– Parity
• Example
– A mirror flips the original object by the vertical
• Parity of mirror = -1.
• Discontinuous symmetry –> No conservation law .
),,(),,(,1
),,(),,(,1
zyxzyx
zyxzyx
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Cross Section• Cross section in particle physics expresses the likelihood
of interaction between two particles.
– Differential cross section, is the probability to observe a scattered particle per unit solid angle.
_ # Particles detected per second_______ _____
(Flux of incident particles)(# target particles)(detector area)
dFN
dN
d
d
t
S
d
d