Status of the Glasgow B→hh analysis CP Working group γ from loops 14 th October 2010 Paul Sail, Lars Eklund and Alison Bates.

Slides:



Advertisements
Similar presentations
Effect of b-tagging Scale Factors on M bb invariant mass distribution Ricardo Gonçalo.
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.
Top Turns Ten March 2 nd, Measurement of the Top Quark Mass The Low Bias Template Method using Lepton + jets events Kevin Black, Meenakshi Narain.
Kevin Black Meenakshi Narain Boston University
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)
8.882 LHC Physics Experimental Methods and Measurements Likelihoods and Selections [Lecture 20, April 22, 2009]
G. Cowan Lectures on Statistical Data Analysis 1 Statistical Data Analysis: Lecture 8 1Probability, Bayes’ theorem, random variables, pdfs 2Functions of.
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.
Fourier Studies: Looking at Data A. Cerri. 2 Outline Introduction Data Sample Toy Montecarlo –Expected Sensitivity –Expected Resolution Frequency Scans:
Analysis Meeting vol Shun University.
 Candidate events are selected by reconstructing a D, called a tag, in several hadronic modes  Then we reconstruct the semileptonic decay in the system.
2 Ready sections (I) 3 Ready sections (II) 4 Sections still in preparation  It would be also worth adding a brief section on possible strategies for.
Status of the Fourier Studies A. Cerri. Outline Introduction Description of the tool Validation –“lifetime fit” –Pulls Toy Montecarlo –Ingredients –Comparison.
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)
CP violation measurements with the ATLAS detector E. Kneringer – University of Innsbruck on behalf of the ATLAS collaboration BEACH2012, Wichita, USA “Determination.
Progress on BR(K L  p + p - ) using a double-tag method A. Antonelli, M. Antonelli, M. Dreucci, M. Moulson CP working group meeting, 25 Feb 2003.
Gavril Giurgiu, Carnegie Mellon, FCP Nashville B s Mixing at CDF Frontiers in Contemporary Physics Nashville, May Gavril Giurgiu – for CDF.
 b Polarization Measurement at ATLAS Michela Biglietti 1 on behalf of the ATLAS  b working group: Eduard De La Cruz Burelo 2, Claudio Ferretti 2, Homer.
Kalanand Mishra April 27, 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,
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
Summary of  2 measurements at Super KEKB Hirokazu Ishino Tokyo Institute of Technology 19 Dec., 2006.
Checks with the Fourier Method A. Cerri. Outline Description of the tool Validation devices –“lifetime fit” –Pulls Toy Montecarlo –Ingredients –Comparison.
Prospects for B  hh at LHCb Eduardo Rodrigues On behalf of the LHCb Collaboration CKM2008 Workshop, Rome, 9-13 September 2008 LHCb.
Charm Physics Potential at BESIII Kanglin He Jan. 2004, Beijing
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)
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
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.
CP Violation Studies in B 0  D (*)  in B A B A R and BELLE Dominique Boutigny LAPP-CNRS/IN2P3 HEP2003 Europhysics Conference in Aachen, Germany July.
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.
Measurements of sin2  1 in processes at Belle CKM workshop at Nagoya 2006/12/13 Yu Nakahama (University of Tokyo) for the Belle Collaboration Analysis.
Measurement of  2 /  using B   Decays at Belle and BaBar Alexander Somov CKM 06, Nagoya 2006 Introduction (CP violation in B 0   +   decays) Measurements.
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.
Julia Thom, FNALEPS 2003 Aachen Rare Charm and B decays at CDF Julia Thom FNAL EPS 7/18/2003 Tevatron/CDF Experiment Decay Rate Ratios and CP Asymmetries.
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.
G. Cowan Lectures on Statistical Data Analysis Lecture 9 page 1 Statistical Data Analysis: Lecture 9 1Probability, Bayes’ theorem 2Random variables and.
Extract the partial rates We can make fits to the partial decay rates to extract (1) normalization f + (0)|V cx | (2) Form factor shape parameters r 1.
Andrzej Bożek for Belle Coll. I NSTITUTE OF N UCLEAR P HYSICS, K RAKOW ICHEP Beijing 2004  3 and sin(2  1 +  3 ) at Belle  3 and sin(2  1 +  3 )
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.
Conditional Observables Joe Tuggle BaBar ROOT/RooFit Workshop December 2007.
Systematics in Hfitter. Reminder: profiling nuisance parameters Likelihood ratio is the most powerful discriminant between 2 hypotheses What if the hypotheses.
Stano Tokar, slide 1 Top into Dileptons Stano Tokar Comenius University, Bratislava With a kind permissison of the CDF top group Dec 2004 RTN Workshop.
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 Bunch length measurement with the luminous region Z distribution : evolution since 03/04 B. VIAUD, C. O’Grady B. VIAUD, C. O’Grady Origin of the discrepancies.
1 D *+ production Alexandr Kozlinskiy Thomas Bauer Vanya Belyaev
Semi-Leptonic B s Mixing at DØ Meghan Anzelc Northwestern University On Behalf of the DØ Collaboration DPF 2006.
Rob Lambert, NIKHEFNikhef 10th February  m blinded analysis of stripping 13 data Rob Lambert and Thomas Bird LHCb-ANA
LNF 12/12/06 1 F.Ambrosino-T. Capussela-F.Perfetto Update on        Dalitz plot slope Where we started from A big surprise Systematic checks.
Searches and limit analyses with the Fourier transform Alex, Amanda, Donatella, Franco, Giuseppe, Hung-Chung, Johannes, Juerg, Marjorie, Sandro, Stefano.
K. Holubyev HEP2007, Manchester, UK, July 2007 CP asymmetries at D0 Kostyantyn Holubyev (Lancaster University) representing D0 collaboration HEP2007,
Erik Devetak Oxford University 18/09/2008
CMSSW_3_1_1 preproduction samples
CP violation in the charm and beauty systems at LHCb
Paul Sail, Lars Eklund and Alison Bates
Vincenzo Vagnoni INFN Bologna CKM Workshop Durham, April 8th 2003
Dilepton Mass. Progress report.
Paul Sail, Lars Eklund and Alison Bates
Paul Sail, Lars Eklund and Alison Bates
Presentation transcript:

Status of the Glasgow B→hh analysis CP Working group γ from loops 14 th October 2010 Paul Sail, Lars Eklund and Alison Bates

2 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

3 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 –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

4

5 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 A dir,mix (B (d,s) →hh).

6 Signal Fraction Fitter Using Toy MC Data

7 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 PDF for each classProb for each class Prob. of a particular event being in each decay class Total mass PDF Mass distribution for each class Total likliehood

8 Signal fractions Use a toy data sample with 1000 data sets, 100k events each data set DecayTrue s/f [%] Initial value [%] Mean fit value [%] Sigma fit value [%] Pull mean* Pull sigma Bd→π+π-Bd→π+π ± ±0.02 B d →K + π ± ±0.03 B d →K - π ± ±0.03 B s →K + K ± ±0.03 B s →K + π ± ±0.03 B s →K - π ± ±0.02 Bd→π+π-π0Bd→π+π-π ± ±0.02 Combinatoric *the pull means are showing a slight bias but this is not a true bias, as will be discussed in the next slide

9 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. B d →π + π - B d →K + π - B d →π + K - B s →K + K -

10 Sensitivity to number of events… continued The sigma of the pull distribution seems fairly independent of the number of events. B d →π + π - B d →K + π - B d →π + K - B s →K + K -

11 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, –B d →π + π - [0.02,0.279] –B d →K + π - [0.125,0.428] –B d →K - π + [0.099,0.354] –B s →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

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

13 CP asymmetry fitter Using Toy MC Data

14 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 A dir (B d →π + π - ) ± ±0.002 A mix (B d →π + π - ) ± ±0.001 A dir (B s →K + K - ) ± ±0.001 A mix (B s →K + K - ) ± ±0.001 B d asymmetries are very well fitted B s 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

15 Time distribution for B d →π + π -

16 Improved B s →K + K - asymmetry fitter Currently the B s →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 B s →K + K - :

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

18 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

19 Outlook Signal fraction 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 Λ b decays into background Asymmetry fitter –Implement and test new analytical PDF for B s decays –Re-express the 4 currently independent asymmetries in terms of d, θ and γ Lifetime fitter –Start rigorous testing in B→hh decays.

20 Thanks

21 Bias in pulls using just statistical uncertainties

22 Back-up Slide Input parametersfor analytic expressions… –Send to Paul on Tuesday

23 Example Asymmetry fits