4 May 2006 First look to the Ke2 decay ● Interesting for the Ke2/k m 2 ratio ● BR(K ±  e n ) = (1.55 ±0.07)10 -5 ● Large radiative decay BR(K ±  e n.

Slides:



Advertisements
Similar presentations
Sabino Meola Charged kaon group meeting 12 October 2006 Status of analysis.
Advertisements

Sabino Meola Charged kaon group meeting 14 December 2006 Status of analysis.
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
STAR Status of J/  Trigger Simulations for d+Au Running Trigger Board Meeting Dec5, 2002 MC & TU.
Barbara Sciascia – LNF 1 K  semileptonic BR measurement B. Sciascia 4 may 2006 KpmKSL joint meeting.
KLOE GM Capri May 2003 K charged status report DE/Dx development vs PiD (next talk by E.De Lucia) →K e3 studies: initial design of efficiency measurement.
Sabino Meola Charged kaon group meeting 12 October 2005 Status of analysis.
1 Search for the Flavor-Changing Neutral-Current Decay,   → p     HyangKyu Park University of Michigan, Ann Arbor for the HyperCP collaboration.
Salvatore Fiore University of Rome La Sapienza & INFN Roma1 for the KLOE collaboration LNF Spring School “Bruno Touscheck”, Frascati, May 2006 CP/CPT.
Claudio Gatti (KLOE Collaboration) LNF INFN K decay measurements with the KLOE detector XXII Rencontres de Physique de La Vallée d’Aoste Feb
14 Sept 2004 D.Dedovich Tau041 Measurement of Tau hadronic branching ratios in DELPHI experiment at LEP Dima Dedovich (Dubna) DELPHI Collaboration E.Phys.J.
Anne Dabrowski Northwestern University Collaboration Meeting 22 nd February 2005 Update Kmu3 Branching Ratio measurement A. Dabrowski, February
1 Outline: Published papers Neutral kaons Charged kaons  decays Hadronic cross section Conclusions Outline: Published papers Neutral kaons Charged kaons.
Measurement of the absolute BR(K  +  -  + ) : an update Patrizia de Simone KLOE Kaon meeting – 21 May 2009.
August 12, 2000DPF Search for B +  K + l + l - and B 0  K* 0 l + l - Theoretical predictions and experimental status Analysis methods Signal.
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.
Particle Identification in the NA48 Experiment Using Neural Networks L. Litov University of Sofia.
Dec 2005Jean-Sébastien GraulichSlide 1 Improving MuCal Design o Why we need an improved design o Improvement Principle o Quick Simulation, Analysis & Results.
Study of the semileptonic decays at 4170 MeV Koloina Randrianarivony Marina Artuso (Syracuse University)
Anne Dabrowski Northwestern University NA48/2 Semileptonics Meeting 22 nd February 2005 Update Kmu3 Branching Ratio measurement A. Dabrowski, February.
B.Sciascia Kpm Meeting - LNF - February, 3 rd Charged kaon meeting LNF - February, 3 rd 2004 B.Sciascia TagBias  Bug on error calculation  Sensitivity.
The Hadronic Cross Section Measurement at KLOE Marco Incagli - INFN Pisa on behalf of the KLOE collaboration EPS (July 17th-23rd 2003) in Aachen, Germany.
Guglielmo De Nardo Napoli University and INFN 7th Meeting on B Physics, Orsay, France, October 4th 2010.
B c Results from CDF II Satyajit Behari (For the CDF Collab.) Johns Hopkins Univ., Baltimore,USA 23 rd Jul HEP2005 Europhysics Conference, Lisboa,
NA48-2 new results on Charged Semileptonic decays Anne Dabrowski Northwestern University Kaon 2005 Workshop 14 June 2005.
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.
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.
K  group activities K + K - retracking features New vs Old : resolution future planning. Conclusion and outlook K + K - retracking features New vs Old.
V.Patera – KLOE GM – Otranto – 10 June 2002 K  reconstruction status K + K - retracking features New vs Old : resolution New vs Old : efficiencies Conclusion.
Barbara Sciascia – LNF 1 Barbara Sciascia Measurement of the absolute branching ratio of K  l3 decays and of the R  e ratio Blessing meeting of the final.
Kalanand Mishra Kaon Neural Net 1 Retraining Kaon Neural Net Kalanand Mishra University of Cincinnati.
25 sep Reconstruction and Identification of Hadronic Decays of Taus using the CMS Detector Michele Pioppi – CERN On behalf.
Measurement of Vus. Recent NA48 results on semileptonic and rare Kaon decays Leandar Litov, CERN On behalf of the NA48 Collaboration.
Study of exclusive radiative B decays with LHCb Galina Pakhlova, (ITEP, Moscow) for LHCb collaboration Advanced Study Institute “Physics at LHC”, LHC Praha-2003,
 0  5  Outline Event selection & analysis Background rejection Efficiencies Mass spectrum Comparison data-MC Branching ratio evaluation Systematics.
PID simulations Rikard Sandström University of Geneva MICE collaboration meeting RAL.
Sabino Meola Kloe meeting 10 March 2005 Status of analysis.
Barbara Sciascia July,29 th - LNF 1 Barbara Sciascia K  semileptonic decays Charged Kaon Meeting July, 29 th - LNF Single photon efficiency in KPM events.
Progress on F  with the KLOE experiment (untagged) Federico Nguyen Università Roma TRE February 27 th 2006.
Status of the hadronic cross section (small angle) Federico Nguyen February 22 nd 2005  the 2002 data sample and available MC sets  trigger efficiency.
Preliminary Measurement of the Ke3 Form Factor f + (t) M. Antonelli, M. Dreucci, C. Gatti Introduction: Form Factor Parametrization Fitting Function and.
Recent results from KLOE Cesare Bini Universita’ “La Sapienza” and INFN Roma 1.The KLOE physics program 2.The KLOE detector 3.Status of the experiment.
B   and B  D ( * )   decays at BaBar Guglielmo De Nardo University of Napoli “Federico II” and INFN Representing the BaBar collaboration 36 th International.
Measurement of the branching ratio of the K +     decay Update E. De Lucia, R. Versaci.
Mike HildrethEPS/Aachen, July B Physics Results from DØ Mike Hildreth Université de Notre Dame du Lac DØ Collaboration for the DØ Collaboration.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
Measurement of the branching ratio of the K +     decay Update E. De Lucia, R. Versaci on behalf of the charged kaon group.
The K L   0  0 decays in KLOE Introduction  pairing Discriminant variables K L   0  0 counting : 3,4,5  ’s samples Control samples for efficiencies.
D. LeoneNovosibirsk, , 2006Pion Form KLOE Debora Leone (IEKP – Universität Karlsruhe) for the KLOE collaboration International Workshop.
1 The use of control channels in the analysis of the B s  μ + μ - decay Tuesday Meeting, 2 June 2009.
Data vs MC … issues of the K +- group 1.Accidentals … contribution from Erika & Roberto 2.DC background.
Guglielmo De Nardo for the BABAR collaboration Napoli University and INFN ICHEP 2010, Paris, 23 July 2010.
Paolo Massarotti Kaon meeting March 2007  ±  X    X  Time measurement use neutral vertex only in order to obtain a completely independent.
KLOE general meeting December 2002 Tor Vergata K charged status report DST production status New analysis items:  K + K - cross section/  line.
M. Martemianov, ITEP, October 2003 Analysis of ratio BR(K     0 )/BR(K    ) M. Martemianov V. Kulikov Motivation Selection and cuts Trigger efficiency.
Electron and Photon HLT alley M. Witek K. Senderowska, A. Żurański.
EXPERIMENTS INR/IHEP Protvino-Moscow, Russia Viacheslav Duk INR RAS BEACH 2006 Highlights on Rare Charged Kaon Decays ISTRA+ & KEK.
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.
Status of the measurement of K L lifetime - Data sample (old): ~ 440 pb -1 ( ) - MC sample: ~125 pb -1 ( mk0 stream ) Selection: standard tag (|
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
Roberto Versaci e + e - collisions from  to  – Novosibirsk /26 1 Charged kaons at KLOE Roberto Versaci on behalf of the KLOE collaboration.
Parameterization of EMC response for
Status of K± p±p0 E. De Lucia.
analisys: Systematics checks
the charged kaon lifetime
Marco Incagli – INFN Pisa
KLOE General Meeting - LNF March,
J/Y Simulations for Trigger
Search for Lepton Flavour Violation in the decay  → BaBar
Presentation transcript:

4 May 2006 First look to the Ke2 decay ● Interesting for the Ke2/k m 2 ratio ● BR(K ±  e n ) = (1.55 ±0.07)10 -5 ● Large radiative decay BR(K ±  e n ) ~ BR(K ±  e ng ) Kinematically very similar to k m 2, that is 10 5 times more abundant. Exploit m /e discrimination in the calorimeter as much as possible The analisys is a less than premature stage. We beg for suggestions, comments, help....

4 May 2006 R K SM = (  0.001)x10 -5 Extremely well known within SM R K SM = (  0.001)x10 -5 Probe  -e universality: non-universal terms from LFV sources in SUSY extensions Preliminary from NA48/2 R K NA48 = (  stat  syst )x signal events from ’03 run and ’04 stat = 2 x stat(2003) not yet included At KLOE the measurement is extremely challenging:  signal =  tag x  rec x  clu ass ~ 8% A possible  /e discrimination strategy can rely on:  decay kinematics (good separation)  TOF (modest separation, also muons have  ~1)  cluster shape in ECAL (could be fairly good, under study)  dE/dx in the DC (could help, under study) c) R K : Ke2/K  2 i.good reconstruction eff. for signal ii.trigger eff. ~ 1 no autotrigger required iii.but difficult PID due to huge K  2 background O(10 5 ) 4x10 3 events/K 2fb -1 OK TRUE

4 May 2006 Starting point ● Possible realistic accuracy achievable with the KLOE statistic ≈ 2% ● The selection sample can be enlarged tagging with the 2 body decay ( as usual) but also with kaon selected by de/dx. 50% gain wrt the usual k  2 tag ● Tag bias and trigger efficiency (no more auto trigger) can be taken under control at 2% level. ● Control sample ??? (mainly for the calorimetric analysis). Partial sovrapposition of energy range with Ke3. Suggestions are welcome (e + e - 

4 May 2006 Momentum distribution ● We use as starting point a sample of K + e2 (full 2fb statistic) using the usual K - m 2 tag as selection. ● MC 2005 was used with the new charged kaon noise inserted ● K+ decay events, tagged by K-m2, reconstructed with vertex in FV Red = MC blu = ke2 black data Lab momentum Mev/c

4 May 2006 Momentun in K center of mass ● We ask for tracks with associated cluster ● To start rejecting the muons we ask for p e *>240 Mev/c ● Total efficiency on the (Ke2+radiative) decay is 15%. (22% if only Ke2 is considered) ● Then we are left with 1700 ev of signal vs 3.3x10 6 k m 2(mc)

4 May 2006 e/m in Ecal ● We would like to push the ECAL rejection relying on the cluster shape. We used first 3 planes where the difference is larger We use the variables: ●  e i =(E i -E i+1 )/(E i +E i+1 ) ● R=E 3 /E 1, ● ●  e max ●  e min MeV N Plane electron muons

4 May 2006 Cut on DE variables ● We ask for the first 3 planes to be on, with energy> 3MeV, and with the cell time within 60 ns from the TOF ● Then we cut on the normalized  E between plane 1 and 2, and between plane 2 and 3  E12  E23 Blu = ke2 red = km2

4 May 2006 Efficiency signal vs bck Cuts legenda : ● 1= tr. Rec. ● 2= clust. Ass. ● 3= p*>240MeV ● 4=  E 12,  E 23 ≠0 ● 5= DE plane cut red=ke2 blu=bck MC purple=data efficiency

4 May 2006 Data vs MC discrepancy.. DATA vs Ke2(MC)BCK(MC) vs Ke2(MC)

4 May 2006 Data vs MC A contribution electron like is present in the DATA Ke2 BCK (MC) DATA Energy(MeV) Plane Energy(MeV)

4 May 2006 Ratio of Ke2/bck eff Cuts legenda : ● 1= tr. Rec. ● 2= clust. Ass. ● 3= p*>240MeV ● 4=  E 12,  E 23 ≠0 ● 5= DE plane cut Rejection= ratio*eff(ke2) Red= on MC blue= DATA Ratio= eff(ke2)/eff(bck)

4 May 2006 After the ECAL rejection: ● Nothing done yet. 1.4x10 5 ev of bck on DATA survive the ECAL cut ev of signal. ● Some distribution are reported (10 pb -1 of data) to spot the useful variables

4 May 2006 About tof..... ● It is not so powerful, since the muons are almost relativistic ( differently from that one of the semileptonic decay..) ● Red = ke2 ● Blu = BCK(MC) ● Dot = DATA

4 May 2006 How to proceed? ● Cut on the reconstructed kink of the muon decaying into electron ● Exploit (?) TOF ● Neural net or likelihood on the calorimetric variables (control samples from data needed!!) ● Finally emiss-pmiss, if the signal can be seen!!