elizabeth worcester university of chicago august 25, 2011 final ktev measurements of cp violation...
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![Page 1: Elizabeth Worcester University of Chicago August 25, 2011 Final KTeV Measurements of CP Violation and CPT Symmetry BNL Particle Physics Seminar For the](https://reader038.vdocument.in/reader038/viewer/2022110321/56649cdc5503460f949a7d54/html5/thumbnails/1.jpg)
Elizabeth WorcesterUniversity of Chicago
August 25, 2011
Final KTeV Measurements of CP Violation and CPT Symmetry
BNL Particle Physics Seminar
For the KTeV Collaboration: Arizona, Campinas, Chicago, Colorado, Elmhurst, FNAL, Osaka, Rice, Sao Paulo, UCLA, Virginia, Wisconsin
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ETW BNL Seminar
Overview
August 25, 2011
CP Violation and CPT Symmetry in KaonsIntroductionCurrent status
KTeV ExperimentDetectorData analysisMonte Carlo simulationFitsSystematic uncertainties
KTeV ResultsFuture of KTeV
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ETW BNL Seminar
Overview
August 25, 2011
CP Violation and CPT Symmetry in KaonsIntroductionCurrent status
KTeV ExperimentDetectorData analysisMonte Carlo simulationFitsSystematic uncertainties
KTeV ResultsFuture of KTeV
Focus on EM showers in CsI
calorimeter
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ETW BNL Seminar
CP Violation and CPT Symmetry
August 25, 2011
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ETW BNL Seminar
CP Violation in Kaons
August 25, 2011
Strangeness Eigenstates:
€
K 0 = sd
K 0 = sd
CP Eigenstates:
€
K1 =1
2K 0 + K 0
( ) CP +1( )
K2 =1
2K 0 − K 0
( ) CP −1( )
Weak Eigenstates:
€
KL ≈ K2 +ε K1 mostly CP −1( )
KS ≈ K1 +ε K2 mostly CP +1( )
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ETW BNL Seminar
CP Violation in Kaons
August 25, 2011
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ETW BNL Seminar
CP Violation in Kaons
August 25, 2011
Indirect CP violation:Discovered in 1964
€
ε =2.2 ×10−3
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ETW BNL Seminar
CP Violation in Kaons
August 25, 2011
Indirect CP violation:Discovered in 1964
€
ε =2.2 ×10−3Direct CP violation:Established in 1999
€
Re ′ ε ε( ) =1.7 ×10−3
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ETW BNL Seminar
Measuring Re(e′/e)
August 25, 2011
1
6
1)Re(
2
00
εε
εε
)(
)(
S
L
KA
KA
εε
2)(
)(00
00
00
S
L
KA
KA
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ETW BNL Seminar
Measurements of Re(e′/e)
August 25, 2011
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ETW BNL Seminar
Measurements of Re(e′/e)
August 25, 2011
Phys.Rev.D83:092001,2011; arXiv:1011.0127
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ETW BNL Seminar
Calculating Re(e′/e)
August 25, 2011
Standard model predicts CP violation through complex phase in CKM matrix
Amplitudes calculated using operator product expansion
10 operatorsW exchangeQCD penguinsEW penguins
Wilson coefficients (short distance physics) well understood at NLO
Large uncertainties in long distance physics
Current predictions 1-30×10-4
Precise lattice QCD calculations expected in the future (R. Mawhinney, Lattice 2011)
Figure courtesy of S. Bertolini.
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ETW BNL Seminar
CPT Symmetry in Kaons
August 25, 2011
€
φ+−≈φε + Im ′ ε ε( )
φ00 ≈ φε − 2Im ′ ε ε( )
Δφ = φ00 − φ+− ≈ −3Im ′ ε ε( )
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ETW BNL Seminar
CPT Symmetry in Kaons
August 25, 2011
€
φ+−≈φε + Im ′ ε ε( )
φ00 ≈ φε − 2Im ′ ε ε( )
Δφ = φ00 − φ+− ≈ −3Im ′ ε ε( )
€
If CPT :
φε = φ ′ ε
Im ′ ε ε( ) = 0
φ+− = φ00 = φSW
φSW = tan−1 2ΔmΓ( )
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ETW BNL Seminar
Measuring Kaon Parameters
August 25, 2011
€
A f t( )2∝ eΓS t + 2Re
cL,0
cS,0
A fL
A fS
e−iΔmt ⎡
⎣ ⎢
⎤
⎦ ⎥e− ΓS +ΓL( )t 2 +
cL ,0
cS,0
2A fL
A fS
2
e−ΓL t
⎧ ⎨ ⎪
⎩ ⎪
⎫ ⎬ ⎪
⎭ ⎪
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ETW BNL Seminar
Measuring Kaon Parameters
August 25, 2011
€
A f t( )2∝ eΓS t + 2Re
cL,0
cS,0
A fL
A fS
e−iΔmt ⎡
⎣ ⎢
⎤
⎦ ⎥e− ΓS +ΓL( )t 2 +
cL ,0
cS,0
2A fL
A fS
2
e−ΓL t
⎧ ⎨ ⎪
⎩ ⎪
⎫ ⎬ ⎪
⎭ ⎪
tS
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ETW BNL Seminar
Measuring Kaon Parameters
August 25, 2011
€
A f t( )2∝ eΓS t + 2Re
cL,0
cS,0
A fL
A fS
e−iΔmt ⎡
⎣ ⎢
⎤
⎦ ⎥e− ΓS +ΓL( )t 2 +
cL ,0
cS,0
2A fL
A fS
2
e−ΓL t
⎧ ⎨ ⎪
⎩ ⎪
⎫ ⎬ ⎪
⎭ ⎪
tS
cos(Dmt + fh)
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ETW BNL Seminar
The KTeV Experiment
August 25, 2011
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ETW BNL Seminar
Bruce Winstein (1943-2011)
August 25, 2011
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ETW BNL Seminar
The KTeV Experiment
August 25, 2011
Collect KL and KS decays to charged and neutral final states simultaneously
Movable active regenerator to provide a coherent mixture of KL and KS and to veto scattered kaons
Charged spectrometer to reconstruct K → p+p decays
CsI calorimeter to reconstruct K → p0p0 decays
Detailed MC simulation to correct acceptance
Collected data in 1996, 1997, and 1999
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ETW BNL Seminar
Regenerator
August 25, 2011
Coherent regeneration: forward direction
Diffractive regeneration: kaon scatters at finite angle
Inelastic regeneration: target nucleus destroyed, secondary particles may be produced
€
KL
€
KL + ρ KS
€
σK 0
> σK 0
Regenerator (r)
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ETW BNL Seminar
Charged Spectrometer
August 25, 2011
4 drift chambersHexagonal cell geometry2 planes each in x and y
Dipole magnet~412 MeV/c kick in x
Calibrated using data and the known kaon massPosition resolution ~80
mmMomentum resolution
~0.3%Absolute momentum
scale ~0.01%
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ETW BNL Seminar
CsI Calorimeter
August 25, 2011
3100 CsI crystals viewed by PMTsSmall crystals
2.5×2.5×50 cm3
Large crystals 5.0×5.0×50 cm3
Calibrated by in-situ laser system and momentum analyzed electrons from Ke3 decaysPosition resolution
~1.2 mm (small crystals)~2.4 mm (large crystals)
Energy resolution ~0.6%Absolute energy scale
~0.04%
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ETW BNL Seminar
K → p+p- Analysis: Reconstruction
August 25, 2011
X vs Z Y vs Z
Tracks bend in analyzing
magnet
Kaon decay vertex
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ETW BNL Seminar
K → p+p- Analysis: Invariant Mass
August 25, 2011
Vacuum Beam
Regenerator Beam
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ETW BNL Seminar
K → p+p- Analysis: PT2
August 25, 2011
Vacuum Beam
Regenerator Beam
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ETW BNL Seminar
K → p0p0 Analysis
August 25, 2011
Only signal is 4
photon showers in
CsI calorimete
r
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K → p0p0 Analysis: Photon Pairing
28
Must determine which photons are from the same pion decay
Pair photons and calculate d for each pair using pion mass as constraint
Only correct pairing will yield consistent d for both pairs
Consistency of measured d quantified by pairing chi-squared variable
Choose incorrect pairing for 0.007% of 2p0 events
€
d12 ≈E1E2
mπ 0
r12
d
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ETW BNL Seminar
CsI Clustering
August 25, 2011
Build clusters around local energy maxima7×7 clusters (small crystals)3×3 clusters (large crystals)
Determine positions by comparing the fraction of energy in neighboring rows and columns
Determine energies by summing crystal energies and applying correctionsEnergy outside clusterEnergy shared between
clustersVariations of CsI responsePhoton-electron differences
7×7 Cluster
Energy outside cluster
Seed crystal
Moliere radius: 3.8
cm
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ETW BNL Seminar
Longitudinal Uniformity Correction
August 25, 2011
Longitudinal response of CsI crystals uniform to ~5%
Response of individual crystals measured in 10 bins using cosmic ray muons passing vertically through CsI
Longitudinal shower profiles generated using GEANT
Longitudinal response of CsI convolved with predicted shower profile for each crystal
Individual crystal energies corrected
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ETW BNL Seminar
Energy Linearity Correction
August 25, 2011
Removes residual energy non-linearity
Measured separately for each crystal using E/p of electrons from calibration sample
Applied multiplicatively to each clusterBased on seed crystalApplied as a function of
cluster energyCorrection generally <
1%
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ETW BNL Seminar
Spill-by-Spill Correction
August 25, 2011
Corrects for global fluctuations in CsI response over timeEg: small temperature changes affect CsI scintillation
propertiesMeasured using E/p of electrons from calibration sampleCorrection < ~0.5%
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ETW BNL Seminar
CsI Performance
August 25, 2011
Calibration based on 1.5 billion electrons from KL → p±e∓n decays
Final E/p resolution after all corrections ~0.6%
E/P resolution
Estimated
momentum
resolution
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ETW BNL Seminar
Final Energy Scale
August 25, 2011
z vertex at regenerator edge
z shift to match data to MC
Before
After
Avg z shift: 2.5 cmAvg energy scale adjustment: 0.04%
1999 Data and MC
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ETW BNL Seminar
K → p0p0 Analysis
August 25, 2011
Reconstructed Invariant Mass
Mass resolution
~1.5 MeV/c2
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ETW BNL Seminar
Monte Carlo Simulation
August 25, 2011
Monte Carlo used to make acceptance correction and to simulate background to signal modesSimulates kaon
generation, propagation, and decay
Simulates detector geometry and response
Much of tracing and detector response based on GEANT libraries
Includes beam intensity effects by overlaying data events selected by an “accidental” trigger
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ETW BNL Seminar
Improvements to MC
August 25, 2011
More complete treatment of particle interactions with matterIonization energy lossImproved BremsstrahlungImproved delta raysHadronic interactions in drift chambers
Improved electromagnetic shower simulationShower library binned in incident particle
angleEffects of dead material (wrapping and
shims) in CsI calorimeter
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ETW BNL Seminar
EM Shower Simulation
August 25, 2011
GEANT shower library 6 energy bins: (2, 4, 8, 16, 32, 64) GeV
Smear energy to match data resolution Select bin using logarithmic interpolation Scale energy in each crystal to desired energy
325 position bins distributed over one octant of central crystal Rotate showers using octant symmetry to cover other 7 octants
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ETW BNL Seminar
EM Shower Simulation (cont.)
August 25, 2011
GEANT shower libraryAngle bins
Photons: 9 bins (0, ±5, ±15, ±25, ±35) mradElectrons: 15 bins (0, ±5, ±15, ±25, ±35, ±45, ±65, ±85) mradSelect bin using linear interpolationCorrect for difference between desired angle and library angle
by shifting transverse positionLibrary Storage
Shower libraries read into memory during MC generationPacking scheme saves shower info with no more precision than
necessaryOne photon library: 150,000+ showers, 33 MbOne electron library: 400,000+ showers, 93 Mb16 different libraries generated for use in distributed computing
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ETW BNL Seminar
EM Shower Simulation (cont.)
August 25, 2011
GEANT shower libraryAngle bins
Photons: 9 bins (0, ±5, ±15, ±25, ±35) mradElectrons: 15 bins (0, ±5, ±15, ±25, ±35, ±45, ±65, ±85) mradSelect bin using linear interpolationCorrect for difference between desired angle and library angle
by shifting transverse positionLibrary Storage
Shower libraries read into memory during MC generationPacking scheme saves shower info with no more precision than
necessaryOne photon library: 150,000+ showers, 33 MbOne electron library: 400,000+ showers, 93 Mb16 different libraries generated for use in distributed computing
New since 2003
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ETW BNL Seminar
Fraction of energy per CsI crystal
2003: Includes transverse energy correction to match data and MCCurrent: No correction required
Improvements: Shower Shape
August 25, 2011
2003
Current
2003 Current
Data/MC ratio
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ETW BNL Seminar
Improvements: Reconstructed Energy
August 25, 2011
2003
Current
2003
Current
Small crystals
Large crystals
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ETW BNL Seminar
Improvements: Reconstructed Energy
August 25, 2011
2003
Current
2003
Current
12 mm mylar wrapping around crystals
Small crystals
Large crystals
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ETW BNL Seminar
Mass vs. Photon Angle
Improvements: Energy Linearity
August 25, 2011
Mass vs. Energy
2003 Current
2003 Current
Data DataData
Data
MC
MC
MC M
C
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ETW BNL Seminar
Improvements: Energy Scale
August 25, 2011
Scale Correction vs. Kaon Energy
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ETW BNL Seminar
Background
August 25, 2011
Scattering background Scattering in defining collimator Diffractive and inelastic scattering in
regenerator Common to charged and neutral modes Characterized using p+p- events with large
pT2
Level higher in neutral mode: no cut on pT2
Use RING variable instead (C.O.E. to beam center)
Non pp background Semileptonic kaon decays in charged mode K → 3p0 decays and hadronic production in
neutral mode Background simulated by MC, normalized
to data sidebands, and subtracted Total background levels
Charged mode: ~0.1% Neutral mode: ~1% K→p0p0 RING,vacuum
beam
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ETW BNL Seminar
Extracting physics parameters
August 25, 2011
Fitter used to apply MC acceptance correction and treat KL-KS interference
Acceptance correction binned in p,z Large correction 85% from geometry
Prediction function calculates decay distributions – nearly identical to MC treatment
Acceptance corrected prediction function compared to background subtracted data using a c2
Minimize c2 using MINUIT Re( e /e)
12 p bins CPT symmetry assumed: f+-= f00= fSW
Kaon parameters and phases 12 p bins, 12 z bins (reg. beam) tS, Dm, fe, Re( e /e), Im( e /e) are fit simultaneously CPT assumption applied a posteriori
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ETW BNL Seminar
Systematic Uncertainties
August 25, 2011
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ETW BNL Seminar
Uncertainty from Background
August 25, 2011
Background Source Systematic Uncertainty in Re(e´/e)(×10-4)
Regenerator Scattering:
High pT2 Acceptance 0.40
K→p+p- Background 0.20
K→p+p- Analysis 0.75
pT2 Fit Procedure 0.30
pT2 Fit Quality 0.40
Charged-Neutral Veto Differences
0.30
Collimator Scattering 0.10
KL→p0p0p0 0.06
Other 0.11
Total 1.06
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ETW BNL Seminar
Uncertainty from Acceptance
August 25, 2011
Quality of MC simulation evaluated by comparing vacuum beam z vertex distributions between data and MC
Bias in Re( e /e) given by sDz/6s: slope of data-MC
ratioDz: difference between
mean z value for vacuum and regenerator beams
Use p+p- and p0p0p0 slopes to determine systematic uncertainty
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ETW BNL Seminar
Uncertainty from Energy Non-linearity
August 25, 2011
Use MK vs. EK plot to determine distortion that provides best data-MC match
Non-linearities:1996: 0.3%/100 GeV1997: 0.1%/100 GeV1999: 0.1%/100 GeV
Change in Re( e /e)1996: -0.1 × 10-4
1997: -0.1 × 10-4
1999: +0.2 × 10-4
Systematic uncertainty: ±0.15 × 10-4
Nominal data
MC
Distorted data
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ETW BNL Seminar
Uncertainty from Energy Non-linearity
August 25, 2011
Use MK vs. EK plot to determine distortion that provides best data-MC match
Non-linearities:1996: 0.3%/100 GeV1997: 0.1%/100 GeV1999: 0.1%/100 GeV
Change in Re( e /e)1996: -0.1 × 10-4
1997: -0.1 × 10-4
1999: +0.2 × 10-4
Systematic uncertainty: ±0.15 × 10-4
Nominal data
MC
Distorted data
Reduced from ±0.66 × 10-4 in 2003
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ETW BNL Seminar
Uncertainty from Energy Scale
August 25, 2011
Check energy scale by studying hadronic interaction events in regenerator and vacuum window
Data and MC match within errors at regenerator
Shifts required to match data and MC at vacuum window1996: -0.81 ± 0.32 cm1997: 1.47 ± 0.19 cm1999: 1.06 ± 0.17 cm
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ETW BNL Seminar
Uncertainty from Energy Scale
August 25, 2011
Total uncertainty: ±0.65 × 10-4
±0.82 × 10-4
±0.59 × 10-4
±0.45 × 10-4
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ETW BNL Seminar
Uncertainty from Energy Scale
August 25, 2011
Total uncertainty: ±0.65 × 10-4
±0.82 × 10-4
±0.59 × 10-4
±0.45 × 10-4
Reduced from ±1.27 × 10-
4 in 2003
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ETW BNL Seminar
KTeV Results
August 25, 2011
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ETW BNL Seminar
Re( e /e) Result
August 25, 2011
€
Re ′ ε ε( ) = 19.2 ±1.1 stat( ) ±1.8 syst( )[ ] ×10−4
= 19.2 ± 2.1( ) ×10−4
Probability: 13%
KTeV 11
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Re( e /e) Result: Crosschecks
August 25, 2011
Run Ranges
Half Samples
Momentum Bins
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Kaon Parameter Results
August 25, 2011
No CPT assumption:Dm = (5279.7 ± 19.5) × 106 ħs-1
tS = (89.589 ± 0.070) × 10-12 s
CPT assumption applied:Dm = (5269.9 ± 12.3) × 106 ħs-1
tS = (89.623 ± 0.047) × 10-12 s
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ETW BNL Seminar
Kaon Parameter Results: Dm and tS
August 25, 2011
KTeV 2003: Dm = (5261 ± 13) × 106 ħs-1
KTeV 2003: tS = (89.65 ± 0.07) × 10-
12 s
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ETW BNL Seminar
Kaon Parameter Results: CPT Tests
August 25, 2011
fe = (43.86 ± 0.63)°fe - fSW = (0.40 ± 0.56)°
Df = (0.30 ± 0.35)°
KTeV + NA48
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ETW BNL Seminar
K0-K0 Mass Difference
August 25, 2011
Use Bell-Steinberger and KTeV measurements to place limit on K0-K0 mass difference (DM)
Non-zero DM → CPT violation
Largest contribution comes from KL,S → p+p- and KL,S → p0p0
DM < 4.8 × 10-19 GeV/c2 (95% C.L., DG = 0)
€
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KTeV Results: Summary
August 25, 2011
Re(ε´/ ε) = (19.2 ± 2.1) × 10-4
Δm = (5269.9 ± 12.3) × 106 ħs-1
tS = (89.623 ± 0.047) × 10-12 s fe = (43.86 ± 0.63)°f e - fSW = (0.40 ± 0.56)°Df = (0.30 ± 0.35)°
GeV/c2 at 95% C.L.
No CPT assumpt
ion
Assuming CPT
Consistent with CPT
symmetry
€
MK 0 − M
K 0< 4.8 ×10−19
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ETW BNL Seminar
The Future of KTeV
August 25, 2011
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ETW BNL Seminar
Dalitz Branching Ratio Measurement
August 25, 2011
€
KL →π 0π 0π 0
e+e−γ
€
B π 0 →e+e−γ( )
B π 0 →γγ( )= 1.1559 ± 0.0116( )%
•E. Abouzaid thesis (U.Chicago)•~60k Dalitz decays•PRD to be submitted this year
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Continuing access to KTeV data
August 25, 2011
http://www.virtualbox.org/
Aging computers difficult/impossible to maintain
Analysis software/computing infrastructure designed for older machines
Data still valuableStored in dCache/Enstore at FNAL
Use VirtualBox to create ‘kopy’ – a virtual Linux machine capable of running KTeV softwareM. Ronquest (LANL)It works!
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ETW BNL Seminar
Dark Photons
August 25, 2011
A´: same interactions as SM photon with reduced coupling
APEX: JLab experiment to search for A´
KTeV search:p0 → gA´→ ge+e-
Signal would appear as resonance above continuum in e+e- invariant mass distribution
Expected sensitivity based on KL→ 3p0
D decays used in measurement of p0→ e+e- branching ratio R. Niclasen thesis (U. Colorado)
R. E
ssig, JLa
b
20
10
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ETW BNL Seminar
Conclusion
August 25, 2011
Re(ε´/ ε) measured to 10%Re(ε´/ ε) = (19.2 ± 2.1) × 10-4
Precise measurements of kaon parameters Dm and tS
Δm = (5269.9 ± 12.3) × 106 ħs-1
tS = (89.623 ± 0.047) × 10-12 s
Phase measurements consistent with CPT symmetry
Precise p0 Dalitz branching ratioB(p0 → e+e-g)/B(p0 → gg) = (1.1559 ±
0.0116)%Dark photons to come?
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Extra Slides
August 25, 2011
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ETW BNL Seminar
Charged Mode Background
August 25, 2011
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ETW BNL Seminar
Charged Mode Background
August 25, 2011
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ETW BNL Seminar
Neutral Mode Background
August 25, 2011
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ETW BNL Seminar
Neutral Mode Background
August 25, 2011
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ETW BNL Seminar
Neutral Mode Background
August 25, 2011
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ETW BNL Seminar
Screening Corrections
August 25, 2011
Regeneration described by power law in fit
Nuclear screening corrections requiredUse elastic and
inelastic modelsCheck corrections
by fitting regeneration amplitude in p bins
Good agreement at low momentum
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ETW BNL Seminar
Screening Corrections
August 25, 2011
For p binned fit, evaluation regeneration phase using Derivative Analyticity Relation (DAR)
Perform fit which floats the regeneration phase in p bins, DAR agrees well with data
Evaluate systematic uncertainty by comparing inelastic screening correction (nominal) to direct fit to data using DAR for the phase
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ETW BNL Seminar
Regeneration
August 25, 2011
€
ρ =iπNLf−g(L)
f− ≡ hf (0) − f (0)
p
f−( p) = f−(70 GeV /c)p
70 GeV /c
⎛
⎝ ⎜
⎞
⎠ ⎟
α
φ f = −π
22 + α( )Analyticit
y
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Regenerator Scattering Background
August 25, 2011
€
d3Nregscat
dpT2dτdpK
= M( pK ) × T(pK ) × S( pK ) × A jeα j pT
2
ˆ ρ jeΛS t +ηeΛL t
2
j =1
6
∑
Malensek energy spectrum
Kaon transmission
Absorber scatter correction
1. Inelastic KS-like scattering
2. Lead scattering3. Single carbon
scattering4. Multiple carbon
scattering5. Hydrogen scattering6. Inelastic KL-like
scattering
€
ϕ ˆ ρ jand α j
For lead scattering, have momentum dependence not explicit in this equation.