rare kaon decay results from e949 at bnl: k + p + n n
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Rare Kaon Decay Results From E949 At BNL: K + p + n n. Shaomin CHEN TRIUMF, Canada. Motivation is clear and simple. To construct the K unitarity triangle and confirm the “golden” relation which is valid in the SM and MFV. - PowerPoint PPT PresentationTRANSCRIPT
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8/16/2004 ICHEP2004, Beijing
Rare Kaon Decay Results From E949 At BNL: K+
Shaomin CHENTRIUMF, Canada
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Motivation is clear and simple
(sin2sinJ/
Ks
Use K+ and K0 to measure the CPV related elements
To construct the K unitarity triangle and confirm the “golden” relation which is valid in the SM and MFV.
A.J. Buras et.al hep-ph/0405132
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Experiment is challenging
Weapons needed to suppress background by 1010
in order to see the signal.
Process EventsK 6343000000K 2113000000K 55000000Beam bkg 25000000Knp, Kl-
46000
K 1 Where can we find such a “WMD”?
Standard Model: Br(K+ 10-10
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BNL-E949 detector -- Rejecting beam backgrounds
e+
Beam backgrounds include pion scattering, kaon decay-in-flight, and charge-exchange reactions.
cerenkov
K cerenkov
B4
K
Top half of side view
Charge exchange
Beam 1
Beam 2
K cluster
cluster
K decay
Target fibres
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BNL-E949 detector -- Powerful and redundant particle ID
Resolutions:P/P ~ 1.1%; R/R~ 3.0%; Rejectionsfor ~for photon with 4 sr coverage.
Top half of end view
-ID from its decay chain.
dE/dxR/P
Photon veto
E787
E949
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This is a team effort!
16 institutes and universities in 4 countries.
…more than 60 physicists from 6 countries.
BNL/FNAL/SBU/UNM, U.S.AIHEP/INR, Russia Fukui/KEK/Kyoto/NDA/Osaka, Japan TRIUMF/UA/UBC, Canada
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Many thanks to BNL-AGS people
Before data taking
After data taking
Twice the instantaneous intensity
Platinum target used in 2002
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Unique Strategy for data analysis
Full data set
1/3 data 2/3 data
Beam bkg
Background study
Background estimate
Step 1
Step 2
Step 3
Step 4
Open the box Step 5E787/E949: we bought a one-way ticket,-no way back after opening the box!
Cuts tuningE787: <0.1 eventE949: <0.5 event
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Background suppression
CutBkg
Kinematics cuts(p/R/E)
Particle ID
Photon veto
Timing cuts
K
K
Beams
Knp, Kl-
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How to achieve a reliable background estimate?
Blind analysis in tuning the cuts. Bifurcated analysis in estimating backgrounds.
1. Form two independent cuts.2. Estimate the background.3. Check the correlation.
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Backgrounds inside the box
Items E949 E787Nk(1012) 1.8 5.9K 0.044 ± 0.005 0.062 ± 0.045K 0.216 ± 0.023 0.034 ± 0.007Beams 0.024 ± 0.010 0.025 ± 0.016Knp, Kl-
0.014 ± 0.003 0.025 ± 0.008
Total bkg (evts) 0.298 ± 0.026 0.146 ± 0.049Errors are statistical only.
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What could be our nightmares?
Correlation between two bifurcated cuts.
A 0.3 event background estimated, but more than 3 events observed!
Appearance of pathology backgrounds.
Underestimating background because…
For example…
It can happen if an observable is used in both CUT1 and CUT2 categories, spoiling the independence of the bifurcated analysis.
It rarely happens but can appear thru a loophole. Hand-scanning the events outside the box is the only way to spot the problem.
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Example1: Correlation between two cuts
Loosen PV x KIN
Obs. Pred.
20 x 20 3 1.820 x 50 8 3.050 x 50 22 11.1
Loosen PV x KIN
Obs. Pred.
20 x 20 4 4.920 x 50 9 12.450 x 50 22 31.1
A new geometrical cut that gained 10% more rejection again 0 was found to
cause trouble in the 1/3 outside-the-box study: N(obs.)~2.0 N(pred.)
retune PV
Reject any event with a photon in opposite side.
Reason: a new cut was developed that used the direction of the + to place a tighter requirement again photons Remedy: remove this cut & retune PV.
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Example 2: Pathology background
K+
K+
B4
Target
Pions scattered back into the target overlaying a non-decaying kaon can make a fake signal.
x
y
zr
Reason: track reconstruction only down to the kaon decay vertex.Remedy: check the hits in the opposite direction of the track.
Readout fibre
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Backgrounds outside the box
Motivations:1) To check the correlations;2) To estimate systematic errors.
Bkg. C Prob. 0.85 0.17 1.15 0.67 1.06 0.40
Fit Nobs. = c Npred.
Npred.
Nobs.
Deviations of c from unity give the systematic errors.
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Acceptance
Br(P.D.G value is 0.211±0.001
Phase space and nuclear interaction effects from Monte Carlo.Acceptance loss due to PID, photon veto, timing and other kinematics cuts directly measured from data.
E949 acceptance: 0.0022 ± 0.002E787 acceptance: 0.0020 ± 0.002
Verification from B(measurements.
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Open the box and guess what?
We see one new event!
E949
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Branching Ratio Result
To make best use of our knowledge of the signal and the background distributions inside the box, we define cells inside the box.
E949 E787
Candidate E949A E787A E787C
S/b 0.9 50 7
W 0.48 0.98 0.88
Br ( 1.47 )10-10
Bi: background of cell containing candidate.Si : Br Ai NK.
NK: Stopped K+’s.Ai: acceptance in a cell.Br: branching ratio.W: S/(S + b).
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Impact on CKM matrix
More data needed for reducing the uncertainty.New neutral kaon experiments (for example KOPIO) expected for further justification.
Many thanks to A. Höcker & J. Ocariz et alThe CKM fitter group, hep-ph/0406184
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Summary
A successful run of E949 with a factor of two more beam intensity as in E787.
A new candidate event observed for K+ , leading to a combined result from E787/E949,
Br(K+ 10-10
~2Br(K+ SM, if (sin2sinJ/Ks.
Statistical fluctuation or evidence of new physics?
hep-ex/0403036