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Se Search arch for for th the e Lep Lepton ton Fl Flavor avor Vio Violating lating De Decay cay in in () Naf afis isa a Tas asne neem em Uni nivers rsity ity of Vic f Victori ria, a, Ca


  1. Se Search arch for for th the e Lep Lepton ton Fl Flavor avor Vio Violating lating De Decay cay in in ๐šฝ(๐Ÿ’๐“) โ†’ ๐’‡ ยฑ ๐‚ โˆ“ Naf afis isa a Tas asne neem em Uni nivers rsity ity of Vic f Victori ria, a, Ca Cana nada. a. On Be Behal alf f of of Ba BaBa Bar r Col olla laboration oration All l Re Resu sults ts Are e Prelimi elimina nary ry The e 2017 17 Divisio vision n of Particles ticles and d Field elds s meeting eting July ly 31 โ€“ Augus gust t 4, 2017 17 Fermi rmila lab, , Ba Batavia via, , IL

  2. Charged Lepton Flavor Violation โ€ข CLFV highly suppressed in SM, allowed in many BSM models + clear exp. signature = โ€œNPโ€ Theoretical constraints on the limit (indirect): BF ( ฮฅ 3๐‘‡ โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ ) < 2.0 ร— 10 โˆ’8 (2000) [1] โ€ข No experimental measurement of the decay ๐œฑ ๐Ÿ’๐‘ป โ†’ ๐’‡ ยฑ ๐‚ โˆ“ yet! โ€ข Some ๐’‡ ยฑ ๐Š โˆ“ ๐’ƒ๐’๐’† ๐‚ ยฑ ๐Š โˆ“ Limits Measurements Results CL (%) Collaboration BF (ฮฅ(3๐‘‡) โ†’ ๐‘“ ยฑ ๐œ โˆ“ ) < 5.0 ร— 10 -6 90 BaBar Collaboration (2010) [2] BF (ฮฅ(3๐‘‡) โ†’ ๐œˆ ยฑ ๐œ โˆ“ ) < 4.1 ร— 10 -6 90 BaBar Collaboration (2010) [2] BF (ฮฅ(3๐‘‡) โ†’ ๐œˆ ยฑ ๐œ โˆ“ ) < 20.3 ร— 10 -6 95 CLEO Collaboration (2008) [3] Indirect Search Provides limit assuming Unitarity Some of the direct experimental bounds from vector particles decay Measurements Results CL (%) Collaboration BF (ฮฆ โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ ) < 2.0 ร— 10 -6 90 SND Collaboration (2010) [4] BF (๐พ/ฮจ โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ ) < 1.6 ร— 10 -7 90 BES III Collaboration (2013) [5] BF (๐‘Ž 0 โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ ) < 7.5 ร— 10 -7 95 ATLAS Collaboration (2014) [6] Direct Search Nafis isa Tasneem eem 2

  3. The BaBar Detector at PEP-II Nafis isa Tasneem eem 3

  4. Data Sample, Signal and Backgrounds Sources of Main Backgrounds ๐‘“ + ๐‘“ โˆ’ โ†’ ๐œ ๐œ Data ฮฅ(3๐‘‡ ) , Luminosity Upsilon Numbers ๐‘ก = 10.355 (fb -1 ) e ฮฝ๐œ‰ (4.06 ยฑ 0.04) ร— 10 6 0.93 ยฑ 0.01 ๐œˆฮฝ๐œ‰ (3%) Pre-blinded Sample (117.7 ยฑ 1.2) ร— 10 6 27.0 2 ยฑ 0.16 Unblinded Sample (121.7 ยฑ 1.2) ร— 10 6 27.96 ยฑ0.16 Removed with kinematics cuts Total MC Signal (for Background) Generators ๐‘“ + ๐‘“ โˆ’ โ†’ ๐œˆ๐œˆ Decayed in flight, ๐‘“ + ๐‘“ โˆ’ โ†’ ๐œˆ + ๐œˆ โˆ’ KK2F Material interaction, e ๐‘“ + ๐‘“ โˆ’ โ†’ ๐‘“ + ๐‘“ โˆ’ Mis-ID etc. BHWIDE ๐œˆ ๐‘“ + ๐‘“ โˆ’ โ†’ ๐œ + ๐œ โˆ’ KK2F ๐‘“ + ๐‘“ โˆ’ โ†’ ๐‘ฃ๐‘’๐‘ก ๐‘“ + ๐‘“ โˆ’ โ†’ e e EvtGen ๐‘“ + ๐‘“ โˆ’ โ†’ ๐‘‘ ๐‘“ ๐‘‘ EvtGen ๐œˆ Generic ฮฅ(3๐‘‡ ) MC EvtGen Mis-ID MC signal: ๐’‡ + ๐’‡ โˆ’ โ†’ ๐œฑ ๐Ÿ’๐‘ป โ†’ ๐’‡ ยฑ ๐‚ โˆ“ : 103000 events Removed with PID Nafis isa Tasneem eem 4

  5. Control Data Sample Luminosity (fb -1 ) Data Purpose ๐ธ๐‘๐‘ข๐‘ ฮฅ(4๐‘‡ ) ๐‘ƒ๐‘œ ๐‘†๐‘“๐‘ก๐‘๐‘œ๐‘๐‘œ๐‘‘๐‘“ , ๐‘ก = 10.58 78.31 ยฑ 0.35 Estimate Continuum Background Preselected as ๐‘“ ยฑ ๐œˆ โˆ“ events Systematics ๐ธ๐‘๐‘ข๐‘ ฮฅ(4๐‘‡ ) ๐‘ƒ๐‘œ ๐‘†๐‘“๐‘ก๐‘๐‘œ๐‘๐‘œ๐‘‘๐‘“ , ๐‘ก = 10.58 78.31 ยฑ 0.35 Systematics Preselected as ๐œˆ ยฑ ๐œˆ โˆ“ events ๐ธ๐‘๐‘ข๐‘ ฮฅ(4๐‘‡ )Off Resonance 7.752 ยฑ 0.04 BG Control Sample ๐ธ๐‘๐‘ข๐‘ ฮฅ(3๐‘‡ )On Resonance , ๐‘ก = 10.355 27.96 ยฑ 0.16 Systematics Preselected as ๐œˆ ยฑ ๐œˆ โˆ“ events ๐ธ๐‘๐‘ข๐‘ ฮฅ(3๐‘‡ )Off Resonance 2.62 ยฑ 0.02 BG Control Sample Nafis isa Tasneem eem 5

  6. Analysis Methodology : A Background filter to select ๐‘“ ยฑ ๐œˆ โˆ“ events Pre-Selec Selection tion: โ€ข User r defin fined ed Sele lection tion: Applied on the pre=selected events โ€ข PID Selecti ection: n: Multivariate Technique applied, 16 different PID selector used in optimization ( ๐ถ ) ๐‘‡ โ€ข Pre-Selection: User defined Selection: Distance of closest approach of any track vertex w.r.t. the beam spot in 2 tracks (1 electron and 1 muon in the final state), one in each Drift Chamber hemisphere, โ€ข in x - y plane < 1 cm and in z < 4 cm. 24 โˆ˜ < ๐œ„ ๐‘€๐‘๐‘ < 130 ยฐ EMC acceptance for both tracks. Number of hits in the Drift Chamber > 0. Transverse Momentum p T > 100 MeV. Exactly 2 oppositely charged tracks ; Lepton momenta must satisfy the following condition Polar angle of the two tracks: 2.8 < ( ๐œ„ 1 + ๐œ„ 2 ) < 3.5 2 2 ๐‘ž ๐œˆ ๐‘ž ๐‘“ ๐‘ก ๐น ๐ถ๐‘“๐‘๐‘› โˆ’ 1 + ๐น ๐ถ๐‘“๐‘๐‘› โˆ’ 1 < 0.01 where ๐น ๐ถ๐‘“๐‘๐‘› = 2 Sum of momentum of the two tracks |P 1 | +|P 2 | > 9 GeV. ๐ท๐‘ > 179 ยฐ Angle between the two lepton tracks must satisfy ๐œ„ 12 One and only one electron of two tracks defined by E/P > 0.8 to ensure they are emerged as back to back. Acolinearity angle associated with the two tracks < 0.1 radians in CM. Energy deposit by Muon track on the Electromagnetic Calorimeter should be greater than 50 MeV. Nafis isa Tasneem eem 6

  7. Data/MC Comparison BaBar Preliminary Distribution of ๐‘“ ยฑ ๐œˆ โˆ“ mass before applying any user defined selection criteria, only preselection criteria has applied for 3% pre-unblinded sample. Nafis isa Tasneem eem 7

  8. Selection Criteria in (N-1) plots (N-1) plots ๏ƒ  all cuts applied except that on the variable plotted BaBar Preliminary BaBar Preliminary 2 2 ๐‘ž ๐œˆ ๐‘ž ๐‘“ ๐น ๐ถ๐‘“๐‘๐‘› โˆ’ 1 + ๐น ๐ถ๐‘“๐‘๐‘› โˆ’ 1 < 0.01 ๐‘ก where ๐น ๐ถ๐‘“๐‘๐‘› = 2 BaBar Preliminary BaBar Preliminary The angle between the two ๐ท๐‘ > lepton tracks must satisfy ๐œ„ 12 179 ยฐ to emerged as back to back. Energy deposit by Muon track on EMC should be greater than 50 MeV. Nafis isa Tasnee eem 8

  9. All Selection Criteria Applied BaBar Preliminary Mass distribution of ๐‘“ ยฑ ๐œˆ โˆ“ after all selection criteria are applied Nafis isa Tasneem eem 9

  10. Data, BG Selection Summary & Signal Efficiency in (N-1) Cuts BG Events ๐‘ช๐‘ฏ ๐‘ญ๐’˜๐’‡๐’๐’–๐’• Can andidate (N-1) Selection Signal Efficiency ๏ฅ eยต ๐œฑ ๐Ÿ’๐‘ป MC ๐œฑ ๐Ÿ“๐‘ป ๐‘ท๐’ ๐œฑ ๐Ÿ’๐‘ป ๐‘ท๐’ (27.02 fb โˆ’1 ) Pre-selection 82612 7134301 152445188 0.2355 ยฑ 0.0013 14.7 ยฑ 2.3 PID selection 0 18 0.2684 ยฑ 0.0012 82.7 ยฑ 6.03 263.4 ยฑ 9.7 Lepton Momentum 302 0.2402 ยฑ 0.0013 0.44 ยฑ 0.44 37.7 ยฑ 3.7 Back to back 39 0.2495 ยฑ 0.0013 13.9 ยฑ 2.2 EMC acceptance 0 17 0.2452 ยฑ 0.0013 17.6 ยฑ 2.5 EMC Energy 0 19 0.2342 ยฑ 0.0013 STAT 12.2 ยฑ 2.1 STAT All Cuts 0 15 โ€ข BG events are the equivalent events on 27.0 fb -1 โ€ข Uncertainties are statistical Note: For the 3% Pre-blinded sample (0.93 fb -1 ): N Data =1, agrees with BG estimate: 0.43 ยฑ 0.07 events Nafis isa Tasneem eem 10

  11. Systematic Uncertainty and Background BaBar Preliminary Systematic Uncertainty on Efficiency: โ€ข Tracking, PID, kinematics, trigger determined using controlled sample of tauโ€™s in the โ€œ Side Bands โ€ where โ€œlepton momentumโ€ and โ€œback to backโ€ cuts are reversed : 1.2% โ€ข Systematic uncertainty on โ€œ lepton momentum โ€ cut: 2.9% โ€ข Systematic uncertainty on โ€œ back to back โ€ cut: 1.1% Systematic Uncertainty on ๐‘‚ ๐‘ (3s ) : [8] Total Uncertainty on ๐‘‚ ๐‘ (3s ) at Run 7 Dataset: 1% โ€ข Source of BG No. of events after all selection criteria Mass distributions for ๏‚ก (3S)On data ฮฅ (4S)On Data: 12.2 ยฑ 2.3 Continuum and MC control samples ( ๏ด -pair) ฮฅ (3S) MC: 0 ยฑ 0.9 Peaking Nafis isa Tasneem eem 11

  12. Summary on Efficiency, Background and Candidate Values Sources Uncertainties ๏ฅ SIG (SYST) โ€ข In the โ€œLepton. Momentumโ€ cut 0.029 โ€ข In the โ€œBack to backโ€ cut 0.011 โ€ข In all other cuts on the Side bands 0.012 ๏ฅ SIG (SYST ๏ƒ… STAT) 0.2342 ยฑ 0.0077 SYST ยฑ 0.0013 STAT 0.2342 ยฑ 0.0078 (4.06 ยฑ 0.04) ๏‚ด 10 6 N ๏‚ก (0.93 fb -1 ) (117.7 ยฑ 1.2) ๏‚ด 10 6 N ๏‚ก (27.02 fb -1 ) 0.42 ยฑ 0.7 Background (0.93 fb -1 ) 12.2 ยฑ 2.3 Background (27.0 fb -1 ) Candidate seen (0.93 fb -1 ) 1 Candidate seen (27.0 fb -1 ) 15 Nafis isa Tasneem eem 12

  13. Results: Branching Fraction and Upper limit ๐‚๐† = ๐‘ถ ๐„๐›๐ฎ๐› โˆ’ ๐‘ถ ๐‘ช๐‘ฏ = (๐Ÿ. ๐Ÿ ยฑ ๐Ÿ. ๐Ÿ“ ๐‘ป๐‘ผ๐‘ฉ๐‘ผ (๐‘ถ ๐‘ฌ๐‘ฉ๐‘ผ๐‘ฉ ) ยฑ ๐Ÿ. ๐Ÿ— ๐‘ป๐’๐‘ป๐‘ผ ) ร— ๐Ÿ๐Ÿ โˆ’๐Ÿ– ๐œป ๐’•๐’‹๐’‰ ร— ๐‘ถ ๐šฝ Measurements Upper Limit with Confidence Level of 90% Observed Upper limit Expected Upper limit ฮฅ(3๐‘‡) โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ Barlow Method [9] CLs Method [10] Barlow Method CLs Method < 3.6 ร— 10 -7 < 3.6 ร— 10 -7 < 2.3 ร— 10 -7 < 2.8 ร— 10 -7 Unblinded Data Sample (27.0 fb -1 ) Nafis isa Tasneem eem 13

  14. Conclusion โ€ข On behalf of the BaBar Collaboration we presented the preliminary result on experimental upper limits of a data sample (27.02 fb -1 ) ๐‘ช๐‘ฎ( ๐œฑ(๐Ÿ’๐‘ป) โ†’ ๐’‡ ยฑ ๐‚ โˆ“ ) < 3.6 ร— 10 -7 with Confidence Level of 90% โ€ข This is the first reported experimental upper limits on ๐›ท(3๐‘‡) โ†’ ๐‘“ ยฑ ๐œˆ โˆ“ Nafis isa Tasneem eem 14

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