Paul Sail, Lars Eklund and Alison Bates

Slides:



Advertisements
Similar presentations
Possible directions for NC sensitivity Philip Rodrigues April 2008 Minos collaboration meeting, Sussex.
Advertisements

Some answers to the questions/comments at the Heavy/Light presentation of March 17, Outline : 1) Addition of the id quadrant cut (slides 2-3); 2)
1/15 Sensitivity to  with B  D(KK  )K Decays CP Working Group Meeting - Thursday, 19 th April 2007 Introduction B  DK  Dalitz Analysis Summary.
Update on NC/CC separation At the previous phone meeting I presented a method to separate NC/CC using simple cuts on reconstructed quantities available.
19th July 2007CPWG1 Model independent determination of γ from B ± →D(K 0 S π + π − )K ± Jim Libby (University of Oxford)
1 Latest CC analysis developments New selection efficiencies: –Based on C++ reco + PDFs rather than old (Fortran+reco_minos) cuts –Attempt to optimise.
Peter Fauland (for the LHCb collaboration) The sensitivity for the B S - mixing phase  S at LHCb.
7/12/2015 Top Pairs Meeting 1 A template fit technique to measure the top quark mass in the l+jets channel Ulrich Heintz, Vivek Parihar.
1 Ghost Trackers If there’s something strange (or charm or bottom) in your neighbourhood… Dave Jackson Oxford University / RAL LCFI Collaboration 28 th.
Pion test beam from KEK: momentum studies Data provided by Toho group: 2512 beam tracks D. Duchesneau April 27 th 2011 Track  x Track  y Base track positions.
Analysis Meeting vol Shun University.
Status of the Glasgow B→hh analysis CP Working group γ from loops 14 th October 2010 Paul Sail, Lars Eklund and Alison Bates.
RooFit toy MC sensitivity studies for  +  s and  m s from B s →D s  /K channels at LHCb Shirit Cohen NIKHEF MSc Colloquium May 11 th 2007.
25/9/2007 LHCb UK meeting 1 ADS determination of γ with B→(Kπ) D K, B→(hh) D K and B→(K3π) D K Jim Libby (University of Oxford)
30th October 2007 LHCb Tuesday Meeting 1 Model independent determination of γ from B ± →D(K 0 S π + π − )K ± Jim Libby (University of Oxford)
3/13/2005Sergey Burdin Moriond QCD1 Sergey Burdin (Fermilab) XXXXth Moriond QCD 3/13/05 Bs Mixing, Lifetime Difference and Rare Decays at Tevatron.
CHARM MIXING and lifetimes on behalf of the BaBar Collaboration XXXVIIth Rencontres de Moriond  March 11th, 2002 at Search for lifetime differences in.
Paul Balm - EPS July 17, 2003 Towards CP violation results from DØ Paul Balm, NIKHEF (for the DØ collaboration) EPS meeting July 2003, Aachen This.
A bin-free Extended Maximum Likelihood Fit + Feldman-Cousins error analysis Peter Litchfield  A bin free Extended Maximum Likelihood method of fitting.
1 Warsaw Group May 2015 Search for CPV in three-bodies charm baryon decays Outline Selections Mass distributions and reconstructed numbers of candidates.
Mitchell Naisbit University of Manchester A study of the decay using the BaBar detector Mitchell Naisbit – Elba.
Mauro Donega’ - CDF collaboration meeting February 3, 2006 B d,s ->h 1 h 2 : BR, CP asymmetries, and lifetimes S. Budroni, S. Donati, M. Donega’, S. Giagu,
Mike HildrethEPS/Aachen, July B Physics Results from DØ Mike Hildreth Université de Notre Dame du Lac DØ Collaboration for the DØ Collaboration.
1 Measurement of the Mass of the Top Quark in Dilepton Channels at DØ Jeff Temple University of Arizona for the DØ collaboration DPF 2006.
Jeroen van Hunen (for the LHCb collaboration) The sensitivity to  s and  Γ s at LHCb.
Kalanand Mishra June 29, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 Giampiero Mancinelli,
Sinéad Farrington University of Glasgow for the CDF Collaboration European Physical Society Aachen, 17 th -23 rd July 2003 B Lifetimes and Flavour Tagging.
Measuring Oscillation Parameters Four different Hadron Production models  Four predicted Far  CC spectrum.
Systematics in Hfitter. Reminder: profiling nuisance parameters Likelihood ratio is the most powerful discriminant between 2 hypotheses What if the hypotheses.
Bc → J/   Lifetime measurement Use 6.7 fb -1 and try two independent approaches Selection 1: no dependence of selection on decay time Fit fixes bkgd.
Paolo Massarotti Kaon meeting March 2007  ±  X    X  Time measurement use neutral vertex only in order to obtain a completely independent.
1 D *+ production Alexandr Kozlinskiy Thomas Bauer Vanya Belyaev
Searches and limit analyses with the Fourier transform Alex, Amanda, Donatella, Franco, Giuseppe, Hung-Chung, Johannes, Juerg, Marjorie, Sandro, Stefano.
23 Jan 2012 Background shape estimates using sidebands Paul Dauncey G. Davies, D. Futyan, J. Hays, M. Jarvis, M. Kenzie, C. Seez, J. Virdee, N. Wardle.
Biagio Di Micco  mass measurement Systematics on   mass measurement Biagio Di Micco.
Update on A FB Myfanwy Liles μ-μ- μ+μ+ q q θ*θ*. A FB Reminder  Forward-Backward Asymmetry  Due to parity violation of the weak interaction  Interference.
Statistical Significance & Its Systematic Uncertainties
Erik Devetak Oxford University 18/09/2008
Inclusive Tag-Side Vertex Reconstruction in Partially Reconstructed B decays -A Progress Report - 11/09/2011 TDBC-BRECO.
B meson studies - from commissioning to new physics effects.
CMSSW_3_1_1 preproduction samples
Hadronic B Decays at BELLE and BABAR
light jet energy scale from Wjj
CP Violating TGCs Tim Barklow July 2, 2003.
Muon momentum scale calibration with J/y peak
Time-dependent analyses at D0-D0 threshold
γ determination from tree decays (B→DK) with LHCb
VELO systematics and physics LHCb VELO meeting, CERN, 28 March 2008
2vtx tagged dijets mass resolution study
Vincenzo Vagnoni INFN Bologna (on behalf of the LHCb Collaboration)
Representing the BaBar Collaboration
Quarkonium production in ALICE
W Charge Asymmetry at CDF
CP violation in the charm and beauty systems at LHCb
W boson helicity measurement
How charm data may help for φ3 measurement at B-factories
CP violation in Bs→ff and Bs → K*0K*0
Prospects for quarkonium studies at LHCb
LHCb Rare Decays Status
Jacopo Nardulli NIKHEF (On behalf of the LHCb collaboration)
Summary of validation studies of the simplified geometry
Top mass measurements at the Tevatron and the standard model fits
Paul Sail, Lars Eklund and Alison Bates
Vincenzo Vagnoni INFN Bologna CKM Workshop Durham, April 8th 2003
Measuring γ at LHCb with Dalitz Methods and Global Sensitivity
Bs Physics and Prospects at the Tevatron
Dilepton Mass. Progress report.
Mixing/Lifetime Needs
Search for
Paul Sail, Lars Eklund and Alison Bates
Presentation transcript:

Paul Sail, Lars Eklund and Alison Bates Status of the Glasgow B→hh analysis CP Working group γ from loops 15th October 2010 Paul Sail, Lars Eklund and Alison Bates

Overview Data selection Introduce Glasgow’s newly developed fitting package called G-Fact. Signal fraction fit results on toy data including sensitivity study on the number of events. Asymmetry fitter using the mass fitter signal fractions as input. Summary and outlook

Data selection Run on X pb-1 from Real Data + Reco06-Stripping10-Merged List of selection cuts: min(piplus_MINIPCHI2, piminus_MINIPCHI2)>30 max(piplus_MINIPCHI2, piminus_MINIPCHI2)>100 min(piplus_PT, piminus_PT)>1500 max(piplus_PT, piminus_PT)>3000 max(piplus_TRACK_CHI2NDOF,piminus_TRACK_CHI2NDOF)<4 B0_PT>2000 B0_IPCHI2_OWNPV<8 && B0_DIRA_OWNPV>0.99995 B0_FDCHI2_OWNPV>625 B0_OWNPV_CHI2/B0_OWNPV_NDOF<1.6 PID Cuts piplus_PIDmu<5 && piminus_PIDmu<5 && piplus_PIDe<2.5 && piminus_PIDe<2.5 && piplus_PIDp<-1 && piminus_PIDp<0 piplus_PIDK<0 piminus_PIDK<0 piplus_PIDK>0 piminus_PIDK>0

Bd→Kπ B→hh Bd→K+π- Bd→K-π+ Bd→π+π- Bs→K+K-

G-Fact Glasgow has developed a stand alone fitting package called G-Fact (Glasgow Fitter of ACp and Time) which can Fit for the signal fraction Then either fit for lifetimes or Adir,mix(B(d,s)→hh).

Fit for signal fractions The signal fractions are fitted for by maximising this total likelihood to find P(class) The signal probability used in subsequent fits is Total likliehood PDF for each class Prob for each class Mass distribution for each class Prob. of a particular event being in each decay class Total mass PDF

Signal fractions Use a toy data sample with 1000 data sets, 100k events each data set Decay True s/f [%] Initial value [%] Mean fit value [%] Sigma fit value [%] Pull mean* Pull sigma Bd→π+π- 8.47 10 8.45 0.13 -0.13±0.03 1.02±0.02 Bd→K+π- 17.82 15 17.84 0.14 0.12±0.03 0.99±0.03 Bd→K-π+ 14.58 -0.02±0.03 1.01±0.03 Bs→K+K- 0.10 0.01±0.03 1.02±0.03 Bs→K+π- 1.62 1 0.07 -0.03±0.04 0.96±0.03 Bs→K-π+ 0.72 0.71 0.05 -0.32±0.03 1.01±0.02 Bd→π+π-π0 15.0 14.98 0.16 -0.11±0.03 Combinatoric 33.32 38 35.02 *the pull means are showing a slight bias but this is not a true bias, as will be discussed in the next slide

Sensitivity to number of events The mean of the pull distribution for the fitted s/f seems to show a bias for large data samples However, the bias in absolute numbers is shown below absolute bias = pull mean * statistical error of fit The bias in absolute numbers is less than 0.1 % if more than 1000 events are used, below that number a measurable bias is seen. Bd→π+π- Bd→K+π- Bd→π+K- Bs→K+K-

Sensitivity to number of events… continued Bd→π+π- Bd→K+π- Bd→π+K- Bs→K+K- The sigma of the pull distribution seems fairly independent of the number of events.

Sensitivity to initial values A study has been performed to test how sensitive the signal fraction fitter is to the initial values given to the fit. Initial values were generated randomly in the following ranges, Bd→π+π- [0.02,0.279] Bd→K+π- [0.125,0.428] Bd→K-π+ [0.099,0.354] Bs→K+K- [0.061,0.25] Combinatoric [0.11,0.35] Conclusions Statistical error is independent of initial fit input values, as expected. Mean of the pull is distributed over ±0.1 for all signal classes and initial values for #events>1000 Bias in pull mean in absolute numbers is Less than 0.1% if #events > 1000 Less than 0.5% if #events > 100 Sigma of the pull distribution is independent of #events and initial values

Asymmetry fitter Currently implemented analytical PDFs using the following expressions for the time class models

Asymmetry Fits Using a toy data sample which contained Generated s/fs of 24% Bd2pipi, 20% Bd2Kpi and 21%Bs2KK events with the rest being combinatoric background. SSB = 0.65 Fit signal fractions used in asymmetry fitter obtained from the signal fraction fitter 1000 data sets with 100k events. Generated Asymmetry Fit input Asymmetry Mean fitted Asymmetry Sigma of Fitted Asymmetry Adir(Bd→π+π-) 0.38 0.32 0.380±0.002 0.061±0.002 Amix(Bd→π+π-) 0.61 0.69 0.604±0.002 0.048±0.001 Adir(Bs→K+K-) 0.1 0.15 0.088±0.002 0.057±0.001 Amix(Bs→K+K-) 0.25 0.3 0.194±0.002 Bd asymmetries are very well fitted Bs asymmetries are not so well fitted since there is no proper time resolution modelled in the fitted as yet and there is a Gaussian smearing in the generation

Time distribution for Bd→π+π-

Improved Bs→K+K- asymmetry fitter Currently the Bs→K+K- asymmetry fitter has no proper time resolution modelled. We have just completed the calculation for the analytical expression for the normalised PDF Which results in the new PDF for Bs→K+K-:

New Bs→K+K- PDF New PDF Old PDF Now need to implement this new PDF in G-Fact and run the asymmetry fitter and study the improvement in the Bs asymmetries

Summary Selection from data looks good Developed new fitting package, G-Fact, for B→hh decays Signal fractions fits are good sensitivity on number of events and initial fit parameters studied using signal fraction fitter Asymmetry fitter well developed and tested Lifetime fitter exists and has been extensively tested in charm area but soon will be developed in B→hh

Outlook Signal fraction fitter Asymmetry fitter Lifetime fitter Verify on MC Run on real data Need to study current PID PDFs which are currently extracted from MC Need to compare mass PDFs from data and MC to extract offsets and scale factors Implement Λb decays into background Asymmetry fitter Implement and test new analytical PDF for Bs decays Re-express the 4 currently independent asymmetries in terms of d, θ and γ Lifetime fitter Start rigorous testing in B→hh decays.

Thanks

Bias in pulls using just statistical uncertainties

Example Asymmetry fits