JOLANTA BRODZICKA Institute of Nuclear Physics, Krakow April 09, 2003 Doubly charmed B decay B ± D0 D0 K ± ( for ~78 fb -1 )

Slides:



Advertisements
Similar presentations
JOLANTA BRODZICKA Institute of Nuclear Physics, Krakow July 09, 2003 Doubly charmed B decays B D*DK ( for ~90 fb -1 )
Advertisements

New Resonance in D 0 K + Andrzej Bozek for Jolanta Brodzicka & Henryk Palka INP Krakow INP KrakowBAM July 15, 2004 Outline : Physics motivations Physics.
J OLANTA B RODZICKA INP, K RAKOW DC March 03, 2004 Doubly charmed B decays B D (*) D (*) K ( for ~140 fb -1 ) D (*) K resonant structure.
D 0 K + mass spectra D 0 K + mass spectra for: for: B + D 0 D 0 K + B + D 0 D 0 K + B 0 D - D 0 K + B 0 D - D 0 K + B 0 D* - D 0 K + B 0 D* - D 0 K + for.
New Resonance in D 0 K + Andrzej Bozek for Jolanta Brodzicka & Henryk Palka INP Krakow INP KrakowBAM July 15, 2004 Outline : Physics motivations Physics.
Properties Use, share, or modify this drill on mathematic properties. There is too much material for a single class, so you’ll have to select for your.
/4/2010 Box and Whisker Plots Objective: Learn how to read and draw box and whisker plots Starter: Order these numbers.
1  1 =.
2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt ShapesPatterns Counting Number.
FACTORING Think Distributive property backwards Work down, Show all steps ax + ay = a(x + y)
Learning to show the remainder
LHCb-Babar Meeting 8 April Paul Soler University of Glasgow and Rutherford Appleton Laboratory A first look at B s J/ in LHCb.
LHCb Alignment 12 th April 2007 S. Viret Coseners Forum « LHC Startup » 1. Introduction 2. The alignment challenge 3. Conclusions.
Introduction  b observation  b search Summary August 28th, 2008W&C Seminar1 August 28 th, 2008W&C Seminar at Fermilab1 Eduard De La Cruz Burelo CINVESTAV.
Break Time Remaining 10:00.
The basics for simulations
Current SM studies CMB. Reports at last meeting W/Z cross-section (CSC) W-mass (CSC) Dibosons (CSC) Minimum bias (CSC) W+charm.
Clock will move after 1 minute
Select a time to count down from the clock above
Measuring the bb cross- section using B  D o X   decays Liming Zhang & Sheldon Stone Syracuse University.
Measurement of the absolute BR(K  +  -  + ) : an update Patrizia de Simone KLOE Kaon meeting – 21 May 2009.
1 Semiexclusive semileptonic B->charmdecays C. Gatto - INFN Napoli A. Mazzacane - Universita’ di Napoli April 10, 2003.
Radia 1 group Mtg, 05/10/2006 D S Selection Loose cut on D s Mbc, Introduction At the 4170, the  * was proven to decay mostly into D * D *, DD *, and.
Sep. 29, 2006 Henry Band - U. of Wisconsin 1 Hadronic Charm Decays From B Factories Henry Band University of Wisconsin 11th International Conference on.
1 Measurement of f D + via D +   + Sheldon Stone, Syracuse University  D o D o, D o  K -  + K-K- K+K+ ++  K-K- K+K+ “I charm you, by my once-commended.
Determination of the J PC of the X(3872) (Reviews of BN800) S.L. Olsen & S.K. Choi Apr 06, 2005 Belle General Meeting.
MC Study of B°  S Jianchun Wang Syracuse University BTeV meeting 06/27/01.
MC Study on B°  S (Status Report) Jianchun Wang Syracuse University BTeV meeting 05/25/01.
CHARM 2007, Cornell University, Aug. 5-8, 20071Steven Blusk, Syracuse University D Leptonic Decays near Production Threshold Steven Blusk Syracuse University.
Update on X(3872) J PC determination Soo-Kyung Choi Stephen L. Olsen Gyeongsang Univ. Univ. of Hawai’i April Fool’s day 2005 Quarkonium group meeting In.
A Method to measure  + /   detection efficiency asymmetry at LHCb Liming Zhang 08/15/07.
MC Study on B°  J/  ° With J/      °     Jianchun Wang Syracuse University BTeV meeting 03/04/01.
Measuring the bb cross- section using B  D o X   decays Liming Zhang & Sheldon Stone Syracuse University.
Measurement of B (D + →μ + ν μ ) and the Pseudoscalar Decay Constant f D at CLEO István Dankó Rensselaer Polytechnic Institute representing the CLEO Collaboration.
Resonances in decay for 400fb -1 DC Meeting April 10th, 2006 J.Brodzicka, H.Palka INP Kraków J.Brodzicka, H.Palka INP Kraków B +  D 0 D 0 K + B +  D.
Outline: (1) The data sample (2) Some news on the analysis method (3) Efficiency revised (4) Background revised (5) Data: spectrum + “phi-curve”
 Candidate events are selected by reconstructing a D, called a tag, in several hadronic modes  Then we reconstruct the semileptonic decay in the system.
Irakli Chakaberia Final Examination April 28, 2014.
Rare B  baryon decays Jana Thayer University of Rochester CLEO Collaboration EPS 2003 July 19, 2003 Motivation Baryon production in B decays Semileptonic.
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)
4/17/2005FOCUS / Doris Kim1 Doris Y. Kim University of Illinois Urbana-Champaign Content ( hep-ex/ , PLB 607 (2005) 233 ) Part I: Theories of charm.
E. De LuciaNeutral and Charged Kaon Meeting – 7 May 2007 Updates on BR(K +  π + π 0 ) E. De Lucia.
K charged meeting 10/11/03 K tracking efficiency & geometrical acceptance :  K (p K,  K )  We use the tag in the handle emisphere to have in the signal.
Observation in BaBar of a narrow resonance in the D + s  0 system at 2317 MeV Roger Barlow Manchester University For the B A B AR Collaboration.
Status of K S   e analysis C. GattiT. Spadaro Selection on data Selection on MC Efficiencies from data, K L   e, K S    ,      , bhabha.
Search for the decay B c  B s  Masato Aoki September 13, B s  J/  channel 1.Pion reconstruction efficiency 2.Cut variables and optimization.
Summary of  2 measurements at Super KEKB Hirokazu Ishino Tokyo Institute of Technology 19 Dec., 2006.
MSSM H 0  3 prong using vertexing at CMS Helsinki b/tau workshop Lauri A. Wendland / HIP.
On quasi-two-body components of (for 250fb -1 ) (for 250fb -1 ) J.Brodzicka, H.Palka INP Krakow DC Meeting May 16, 2005 B +  D 0 D 0 K + B +  D 0 D 0.
Resonances in decay Resonances in decay (for 400fb -1 ) (for 400fb -1 )BAM February 27th, 2006 J.Brodzicka, H.Palka INP Kraków J.Brodzicka, H.Palka INP.
Study of pair-produced doubly charged Higgs bosons with a four muon final state at the CMS detector (CMS NOTE 2006/081, Authors : T.Rommerskirchen and.
New Resonances at Belle Jolanta Brodzicka INP Kraków, for the Belle Collaboration ICFP 2005 October 4 th, 2005 Taiwan Outline  ‘ old’ X(3872) properties.
Status of vertex efficiency evaluation Fabio Ambrosino, Patrizia de Simone, Paolo Massarotti, Vincenzo Patera the idea is to look for events where the.
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.
Charged Particle Multiplicity, Michele Rosin U. WisconsinQCD Meeting May 13, M. Rosin, D. Kçira, and A. Savin University of Wisconsin L. Shcheglova.
Σ Eγ comparison using Woochun Park Univ of South Carolina Feb 26,
Tomas Hreus, Pascal Vanlaer Overview: K0s correction stability tests Jet-pt correction closure test Study of Strangeness Production in Underlying Event.
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,
Kalanand Mishra February 23, 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 decay Giampiero.
Elliptic flow of D mesons Francesco Prino for the D2H physics analysis group PWG3, April 12 th 2010.
Tomas Hreus, Pascal Vanlaer Study of Strangeness Production in Underlying Event at 7 TeV 1QCD low pT meeting, 18/03/2011.
Processing large data sets Brad Abbott. Now J/Psi Starting with root-tuples Add 4-momentum to look for candidates Pick events (raw) -> reconstruct event.
1 The use of control channels in the analysis of the B s  μ + μ - decay Tuesday Meeting, 2 June 2009.
Measurements of  at LHCb Mitesh Patel (CERN) (on behalf of the LHCb Collaboration) 14th December 2006.
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.
LPNHE Richard Kass December Measurement of the Branching Fraction of B - → D 0 K* - J. Chauveau, M. John, R. Kass, G. Thérin Details of this.
M. Martemianov, ITEP, October 2003 Analysis of ratio BR(K     0 )/BR(K    ) M. Martemianov V. Kulikov Motivation Selection and cuts Trigger efficiency.
Search for Invisible Higgs Decays at the ILC Ayumi Yamamoto, Akimasa Ishikawa, Hitoshi Yamamoto (Tohoku University) Keisuke Fujii (KEK)
Charm Form Factors from from B -Factories A. Oyanguren BaBar Collaboration (IFIC –U. Valencia)
Status of the measurement of K L lifetime - Data sample (old): ~ 440 pb -1 ( ) - MC sample: ~125 pb -1 ( mk0 stream ) Selection: standard tag (|
Presentation transcript:

JOLANTA BRODZICKA Institute of Nuclear Physics, Krakow April 09, 2003 Doubly charmed B decay B ± D0 D0 K ± ( for ~78 fb -1 )

JOLANTA BRODZICKA April 09, 2003 B DDK Analysis details at least 5 good tracks : abs(IP_dz)< 5cm abs(IP_dr)< 0.4cm R 2 < 0.3 K ± : P( K/ ) > 0.4 ± : P( /K ) > 0.1 D 0 reconstruction (see my December ICPV talk for details) B ± D 0 D 0 K ± reconstruction : B vertex fit: with IP and B lifetime constraints, cl_B > 0 (except B decays with D 0 K 0 ) no cos THR, cos PROD shape cuts M bc > 5.2 GeV < E < 0.35 GeV BF ~ 28% ( K, K3, K 0, K s, K s KK, KK ) M (D REC ) cut: ± 20MeV ( D 0 K 0 : ± 50MeV) vertex fit (conf_level>0.), mass constraint fit

JOLANTA BRODZICKA April 09, 2003 B DDK best B candidate choice method (see my December ICPV talk for more details) B(M D ) LR_D (M D ) LR_D (M D ) = S(M D ) + D probability : S(M D ), B(M D ) parameterization from M D fit B probability for B ± D0D0BK ± : LR_B = LR_D 1 × LR_D 2 best B candidate : with max LR_B best = 82 % (for (kpi)(kpi) ) (estimated from rejected MC events DE, Mbc distributions and correlations between accepted and rejected B candidates ) for B ± D0D0BK ± (kpi)(kpi) reconstr. eff is 15% efficiency lost due to B_best choice method is 0.9% choice method efficiency

JOLANTA BRODZICKA April 09, 2003 B DDK B ± D0 D0B K ± D0,D0B K Mbc signal box: abs( E)<25MeV Mbc>5.265 GeV S=28.7±6.5 BF = ( 1.53 ± 0.35 ) * = 15.0% eff = 2.21 * N/2MeV E N/7.5MeV

JOLANTA BRODZICKA April 09, 2003 B DDK B ± D0 D0B K ± LR > 0.04 signal box: abs( E) GeV ( for K 0 –45< E<25MeV ) S=68.6 ± 16.4 BF = ( 1.64 ± 0.39 ) * eff = 4.91 * E N/7.5MeV N/2MeV Mbc

JOLANTA BRODZICKA April 09, 2003 B DDK B ± (3770) K ± hypothesis (3770) D0 D0B MASS D0D0B for signal_box events S = 2.2 ± 2.5 N/14MeV fitted function: BW+sqrt(1-thr/x)*pol_3 BW position and width fixed to nominal (3770) values D0,D0B K LR > 0.04 M(DD) resolution at (3770) region reconstructed M(D0D0B) for spike generated ~1.MeV N/0.25MeV S = 15.9 ± 6.2

JOLANTA BRODZICKA April 09, 2003 B DDK MASS D0D0B for 3body MC B ± D0 D0B K ± D0,D0B K 20MeV bins reconstruction efficiency vs. Mass (D0D0) for 2body MC B ± (3770) K ± D0,D0B K MASS D0D0B = 15.0% = 16.0% 2MeV bins correct now! (Previously wrong generated M(DD) distributions)

JOLANTA BRODZICKA April 09, 2003 B DDK B ± D0 D0B K ± E distributions vs. M(D0D0B) LR>0.02

JOLANTA BRODZICKA April 09, 2003 B DDK B ± D0 D0B K ± E distributions vs. M(D0D0B) projections LR>0.02

JOLANTA BRODZICKA April 09, 2003 B DDK E projections for different M(D0D0B) 80MeV regions LR>0.02

JOLANTA BRODZICKA April 09, 2003 B DDK B ± D0 D0B K ± fitted signal in each M(DD) 80MeV bin LR> lost signal box (partially reconstructed D*D*K ) ( fully reconstructed DDK ) 1 st bin Psi(3770) region: 19 ± 6 lost signal box (partially reconstructed D*DK ) M(D0D0B) Signal\80MeV