Open issues of the pp ee analysis
description
Transcript of Open issues of the pp ee analysis
Open issues of the ppee analysisMauro Raggi, LNF INFN
30th August 2014
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Outline Possible analysis strategies
Addition BG suppression BG evaluation for different strategy
Radiative correction treatment Signal (no correction vs Photos+coulomb) Normalization (Photos+gatti vs Gatti only)
Measuring the BR Total OR IB only or model independent?
Mee systematic checks New cuts vs old cuts.
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Analysis definitions cuts (presel) Good Vertex
-1000 < ZVTX < 8000
NVTXtrk = 3
Good Track TrackQual >0.75 new 2 GeV <TrackP< 60 GeV 12 cm <RDCH1<135 cm 12 cm <RDCH4<135 cm Ddead > 2 cm Track to track dist > 2cm
Good Clusters 2GeV < ECl <60 GeV
accep(LKR) routine for geometrical acceptance Cluster to cluster > 10cm Cluster status <4 new
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Common preselection
Preselection cuts (common to PPD and signal analysis) NgoodVertex=1 3 < NgoodCluster < 8 3 < NgoodTracks < 8 Ellipse 3pc cut 116ns < Track time <154ns 3 good track are the same used in vertex fitting
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Signal selection ngoodCl ≥4
N electrons =2 E/P>0.85
N pions =1 E/P<0.85
N gammas =2 cluster with no associated track &Ecl>3 GeV
COG < 2 cm
abs(ETOT-pk)< 6 GeV
abs(Mpi0-MPI0PDG)<10 MeV
Mee > 0.001022 GeV
Distance of electrons @ DCH1 > 0.25 against conversions
Total charge of electrons = 0
abs(Meeg-MPI0PDG)>0.005 moved to 7MeV) cut on Dalitz decays
Mpp > 0.12 GeV new rejects most of 3pD
abs(MK-MKPDG) < 10 MeV 28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Additional suppression of the BG
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Mee for the two set of cuts
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
BG acceptances comparison
28 August 2013
BG type Acc Old Acc New Nbg old Nbg new
K2pD 4E-7 1.9E-7 76 31
K3pD 6.2E-6 9.8E-7 201 36
Total BG 277.7±17 67±8
DE events 176±13 103±11
Nppee-BG 2540 2175
BG % of sig
~11% 3.1%
Syst error 0.68% 0.37% Adding the Mpp>120 MeV and abs(Meeg) >7 MeV Background is reduced by factor 3.5 The acceptance loss is ~15% Data MC comparison improves BG systematics to the BR goes down to 0.37%
Becomes a BR(ppee)Mpp>120
Needs extrapolation in the full kinematic range to be performed Introduce a cut in the definition of Ntot for the acceptance
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Rad. Corr. flux measurement
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
The Kaon flux measurement
Used the decay K±->p±p0D(g) (PPD) means K±->p±ge+e-(g)
Same trigger chain of the signal
MonteCarlo generator used: Due to radiative correction issue sing several MC generators We have KLOE, MS, Prague with no extra photons We have Gatti+Photos with extra photons generation ppD selection very sensitive to extra photons BG to ppee very sensitive to extra photons as well
Normalization BR used in the calculation: BR(K->2p(g))xBR(p->Dalitz)=(20.66*1.174)x10-
2=(2.425±0.073)x10-3
Flux measurement formula: (NPPD - NBGPPD)/(ePPD x AccPPD x BRPPD)
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
PPD selection cuts N electrons = 2 (0.9<E/p and P > 3 GeV) with different charges
Pion charged = 1 (E/p<0.85 P > 10 GeV)
N gammas = 1 (no ass cluster and E >3 GeV)
COG< 2 cm
abs(M(eeg)-MPI0(PDG)) < 10 MeV
Distance of e+e- tracks at DCH1 > 0.25 cm
abs(ETOT-PK)< 6 GeV
Track and clusters in 5ns (data only)
abs(MK-MK(PDG)) < 10 MeV
T*p > 85 MeV
Mee>10 MeV (new improve data MC agreement)
Trigger (2VTX or 1VTX or 1TRKP)28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Rad. Corr models acceptances
28 August 2013
Model p+p0
P0D
modExtra
gNtot GEN
Ntot Sel
Acc Delta
Gatti Photos Yes 1.558E8
5540701
3.555% 0
Gatti only None No 3.87E8 1.421E7
3.669% 3.2%
Gatti MS No 3.77E8 1.392E7
3.682% 3.6%
Gatti Prague No 3.78E8 1.392E7
3.695% 3.9%
Rad. Correction systematic Generation of extra photons give a 3.2% difference in the acceptance Assuming photos to have a 10% accuracy we propose 0.35% systematic
Absence of the Dalitz plot reweighting on our MC We assume the maximum effect is None-Prague (0.7% systematic)
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Rad correction and BG to ppee
28 August 2013
Old selection
P0D
modExtra
gAccBG NBG BG%
Gatti Photos Yes 4.04E-7 76 3%
Gatti only None No 2.5E-7 47 1.9%
Gatti MS No 2.8E-7 53 2.1%
Gatti Prague No 2.6E-7 49 1.9% With the old selection we have
Maximum difference in the BG evaluation of 29 event ~ 1.1% systematic
new selection
P0D
modExtra
gAccBG NBG BG%
Gatti Photos Yes 1.9E-7 36 3%
Gatti only None No 2.6E-7 49 1.9% With the new selection we have
Maximum difference in the BG evaluation of 13 event ~ 0.6% systematic
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Flux calculation results 2003Quantity Present value Value was Rel Error
BR(p+p0D(g)) (2.425±0.073)x1
0-3 (2.425±0.073)x10-3
3%
Acceptance (3.555±0.0015)%
(8.00± 0.002)% 0.02%
Trigger efficiency (97.64± 0.044)% 97.15 ± 0.042 0.046%
BG in PPD sample 3365 13130 0.1% (Sys)
Ntot events 6714917±2591 14654994 0.038%
Syst rad correction 0.76% 0 0.76%
28 August 2013
Kflux=(7.971±0.03Stat±0.06Sys±0.24Ext)x1010=(7.971±0.25)x1010
was (7.766±0.23)x1010
Error completely dominated by external error dBR(p0
D)=3%Effect of the radiative corrections taken into account
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Radiative corrections ppee
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Radiative corrections on ppee
D’ambrioso papers does’nt include any kind of radiative corrections in the IB martix element and BR evaluation
We implemented the Photos into the IB generator of ppee (many thanks to Brigitte) Include the radiative corrections due to e+e- interaction We also included Coulomb corrections which are constant
We will estimate the systematic due to radiative correction by comparing the acceptance of corrected and non corrected MC The acceptance are:
Rad corr (new sel)= 6.61E-3 with no rad 6.92E-3 -> 4.5% difference
Rad corr (old sel) = 7.44E-3 with no rad 7.81E-3 -> 4.7% difference
Assuming photos to have a 10% accuracy we propose 0.45% systematic
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Mee systematic check
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Mee systematic check
28 August 2013
0 BR(Ppee) 4.19E-06 +/- 8.84E-08 (Nevent 22470 MinCut 1.00E+00 error 2.11E-02)1 BR(Ppee) 4.24E-06 +/- 3.11E-08 (Nevent 21080 MinCut 2.00E+00 error 2.18E-02)2 BR(Ppee) 4.30E-06 +/- 4.81E-08 (Nevent 19140 MinCut 3.00E+00 error 2.29E-02)3 BR(Ppee) 4.30E-06 +/- 6.09E-08 (Nevent 17140 MinCut 4.00E+00 error 2.42E-02)4 BR(Ppee) 4.32E-06 +/- 6.87E-08 (Nevent 15680 MinCut 5.00E+00 error 2.53E-02)5 BR(Ppee) 4.29E-06 +/- 7.54E-08 (Nevent 14290 MinCut 6.00E+00 error 2.65E-02)6 BR(Ppee) 4.25E-06 +/- 8.06E-08 (Nevent 13120 MinCut 7.00E+00 error 2.76E-02)7 BR(Ppee) 4.26E-06 +/- 8.43E-08 (Nevent 12260 MinCut 8.00E+00 error 2.86E-02)8 BR(Ppee) 4.31E-06 +/- 8.70E-08 (Nevent 11600 MinCut 9.00E+00 error 2.94E-02)
Trigger correction not icludedOffset on the BR
Max effect (4.32-4.19)/4.32 ~ 3%
Preliminary Check with new selection
Result independent of the selection type depend on the MC only
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
DE component fitting
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
DE and IB in the Mee spectrum
Difference on the spectrum is very little in the NA48/2 acceptance
G. D’Ambrosio theoretical paper does’nt provide proper treatment of radiative corrections for the IB that are greater than the DE effect itself due to the 2 electrons in the final state
BG is 3 times bigger than the DE component need a fit with Data, IB, DE, INT, BG(2pd), BG(3pD) too many distributions
Much better conditions expected in NA62 104 rejection of the BG due to photon veto 10-20 times more statistics expected
Needs in any case improved theoretical description to get a result.
28 August 2013
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Fitting the DE Fitting the DE using Mee is quite hard for different reasons:
IB and DE distributions of Mee are very similar much more wrt ppg Regions where the DE is dominant are populated by 10% BG The low statistics does’nt allow to have a very hard selection cuts
Seems that our acceptance spoils the difference even more
28 August 2013
IB MC GENDE MC GEN
Before the selection After the selection
IB MC GENDE MC GEN
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Real life is even harder…
28 August 2013
IB MC RECDE MC REC
Reconstructed MC after correct DE normalization including higher acceptance factor 5
Mee
T*p
Situation in T*pi looks a bit betterbut BG has to be taken into account…
IB MC DE MC
IB MC DE MC
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Errors summary table preliminary
28 August 2013
Systematic Value
N of signal events (2450) 2.11% sqrt(2243)/2243
Signal acceptance 0.2%
Total Statistical 2.12%
Difference of 2 analysis 0.45%
Back ground subtraction 0.7% +0.6% (0.35% new selection)
Trigger efficiency 0.65% (From data loose sample)
Non linearity <1%
Radiave correction 0.5 %
Mee 3% to 1% depending on the cut
Total systematics 1.32% + Mee
BR(p0D) external Flux 3.1%
Total external 3.1%
Total Error
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
BR calculations options
Theoretical prediction from G. D’Ambrosio et al (Eur. Phys. J. C (2012) 72:1872):
BR(ppee)IB= 4.19 x 10-6 IB only no isospin correction (PUBLISHED)
BR(ppee)IB= 4.10 x 10-6 IB only isospin breaking correction (PRIVATE)
In the IB only BR we considered DE as a BG we subtracted: DE systematic subtraction to be understood
Model independent BRtot?
28 August 2013
What error for accTot?
Mauro Raggi - I.N.F.N. - Laboratori Nazionali di Frascati - Italy
Conclusions
We improved a lot the analysis agreement between me and Milena
We developed new strategy for BG subtraction
We included the treatment of radiative corrections in both analysis
The comparison with theory is biased by absence of radiative correction in the theoretical paper.
28 August 2013
Thank you for your attention28 August 2013