Search for ≥ 7 Pion Decays of the τ-Lepton with BABAR Richard Kass The Ohio State University ttag trec Introduction t- 7-prongs nt inclusive analysis t- 4p- 3p+ (p0) nt exclusive: 4p- 3p+ nt & 4p- 3p+ p0 nt t- 3p- 2p+ 2p0 nt t- 2wp- nt Results and Conclusions Richard Kass TAU06 Sept 19 2006 1 Motivation for Searches τ decays with ≥ 7 pions have never been observed We have a lot more statistics than previous experiments (× (50-200)) Better understanding of strong interactions in hadronic τ decays resonant substructure exotic resonances ? Potentially useful bound on nt mass if the decay is observed Mt - M2wp =74 MeV Richard Kass Multi-pion t decays are important ! TAU06 Sept 19 2006 2 t- 4p- 3p+ (p0) nt Previous Experiments: HRS (1987): BR < 2.9 × 10-4 PRD 35, 2269 OPAL (1997): BR < 1.8 × 10-5 PL B404, 213 CLEO (1997): BR < 2.4 × 10-6 PRD 56, 5297 Theory: 3 d pn 1 d p1 4 4 d = | M |2 ... ( 2 p ) ( p0 - p1 - ... - pn ) 3 3 2E 0 (2p ) 2 E1 (2p ) 2 En 3 amplitude (dynamical factor) phase space (kinematical factor) BR (t 7pt ) = 10 -3 6 10 -6 BR (t 5pt ) S. Nussinov, M. Purohit, Phys.Rev.D.65 034018 (2002) Richard Kass TAU06 Sept 19 2006 BR (t 7pt ) = 6 10 -12 Provided the decay does not go via resonances 3 t- 3p- 2p+ 2p0 nt Previous Results: No 7p: BR (t 5p2p0 nt) < 1.1×10-4 CLEO PRL, 73, 934 (1994) But 6p has been measured: BR (t 5pp0 nt) = (1.7±0.3)×10-4 CLEO PRL 86,4467 (2001) BR (t w3pnt) = (1.2±0.2)×10-4 ppp0 Theory: No theoretical prediction of the decay rate The decay will most likely go through w meson If w meson dominates the 7-pion decays, t 5p2p0 nt will most likely have the largest BR The decay is likely to go through (2wpnt ) channel (t 5p 2p 0t ) = 2wp 1 8 18 3 3 7p 5p 2 3p 3 p w 2p 35 35 35 10 5 R. Sobie, Phys. Rev. D. 60 017301 (1999) Richard Kass TAU06 Sept 19 2006 4 Data Collection at PEPII The analyses presented here use 232 fb-1 of data* =206.6x106 τ-pairs Collected at CM energy ~ 10.58 GeV *BaBar has collected a total of ~390 fb-1 Richard Kass TAU06 Sept 19 2006 5 Event Pre-Selection Criteria Reject background and reduce size of data samples. 2 < Nch.trk < 11 in event Event divided to 2 hemispheres perpendicular to thrust Thrust magnitude > 0.9 8 (6) well-measured tracks in event, with 1 track recoiling against 7: 1-7 topology (1-5 topology). Zero net charge No g conversions (Me+e< 5 MeV, DXY < 2cm) Rejected 99.95% xis of bkg., a t andth 77% rus of signal p0 g BR(7p/7pp0)=210-5 g No loopers (tracks trapped in B-field) Well-measured photons X e+ e- 1 (2) reconstructed p0’s on signal side 7pp0 (5p2p0) Lots more bkg. to reject Richard Kass TAU06 Sept 19 2006 6 Background Suppression Against qq p-mesons on signal side Against t bkg pT >100 MeV/c on signal side Residual energy on the signal side < 300 MeV DOCAXY / pT < 0.7cmc/GeV on signal side 1-prong tags: e, m, , h+0g 1.3 < Pseudo-Mass < 1.8 GeV/c2 invariant mass Use Pseudo-mass instead of Invariant mass Assume: n is massless & τ direction is given by 7 tracks m*t2= 2(Ebeam – E7p)(E7p – P7p)+m7p2 BR = 210-5 Signal region: 1.3 < M7p < 1.8 GeV/c2 pseudo-mass background shifts upwards with pseudo-mass Shape of pseudo-mass distribution well modeled by MC Richard Kass TAU06 Sept 19 2006 7 t- 4p- 3p+ (p0) nt qq Background Estimate After all cuts (DATA) After preselection (DATA) BABAR fit m, s signal region BABAR extrapolate integrate Fit from 1.8 to 2.6 GeV/c2 after pre-selection with a Gaussian function Extrapolate the fit below 1.8 GeV/c2 Integrate from 1.3 to 1.8 GeV/c2 Use these fit parameters on the final pseudo-mass spectrum. Mean and sigma do not vary significantly throughout the cuts Richard Kass TAU06 Sept 19 2006 8 t- 4p- 3p+ (p0) nt qq Background Estimate Validation Validation on: 1–8 topology data (after all cuts) 1) 1-8 data: 1.3 – 1.8 GeV/c2 region (pure qq background) Cuts 1-8 data 1-7 data exp. obs. exp. obs. Preselection 19.0 ±2.7 23 3356 ±79 3238 7-prong p ID 12.2 ±1.6 10 1503 ±40 1415 7-prong pT 6.7 ±0.8 8 1092 ±30 1103 DOCAXY/pT 2.7 ± 0.3 1 656 ±18 642 1-prong tag 0.5 ± 0.1 0 114 ± 4 106 Good agreement! Richard Kass TAU06 Sept 19 2006 1–7 topology data (after all cuts) validation region 2) 1-7 data: 1.8 – 2.0 GeV/c2 region validation region BABAR BABAR 9 t bkgd. Signal Efficiency t- 4p- 3p+ (p0) nt Systematic Error Estimate Tracking efficiency Particle ID 1-prong generic t BR Limited MC statistics 5.2 % 2.7 % 0.5 % 0.7 % Total uncertainty of signal efficiency (%) 6.0 % Limited t MC statistics t 5pp0nt branching ratio t 5pnt branching ratio 75 % 15 % 7% Total uncertainty of t background (%) 77% qq bkgd. 1.3 ± 1.0 events Fit parameters (%) Num. events fitted (%) Fit range (%) 3.4 % 2.0 % 0.1 % Total uncertainty of qq background (%) 4.0 % 20.3 ± 0.8 events Luminosity and tt- cross-section Richard Kass TAU06 Sept 19 2006 2.3 % 10 t- 4p- 3p+ (p0) nt Results t- 4p- 3p+ (p0) nt eff. (9.4 ± 0.6) % Expected tt- bkg. 1.3 ± 1.0 Expected qq bkg. 20.3 ± 0.8 Total expected bkg. 21.6 ± 1.3 Observed events signal region 24 No evidence for signal ! Sensitivity (Nexp=Nobs) < 2.5 × 10-7 @ 90% CL Branching ratio signal region < 3.0 × 10-7 @ 90% CL Calculated using Bayesian approach Richard Kass TAU06 Sept 19 2006 11 Exclusive t- 4p- 3p+ nt Background estimate method is identical to t - 4p- 3p+ (p0) nt case Additional cut: no g’s on the 7-prong side. t- 4p- 3p+ nt eff. (5.5 ± 0.3) % Expected tt- bkg. 0.8 ± 0.8 Expected qq bkg. 3.1 ± 0.1 Total expected bkg. 3.9 ± 0.8 Observed events BABAR signal region 8 signal region No evidence for signal ! Sensitivity < 2.2 × 10-7 @ 90% CL Branching ratio < 4.3 × 10-7 @ 90% CL Richard Kass TAU06 Sept 19 2006 12 Exclusive t- 4p- 3p+p0 nt Require 1 reconstructed p0 on the 7-prong side: BABAR 113 < Mgg < 155 MeV/c2 t- 4p- 3p+ p0 nt eff. (3.6 ± 0.3) % Expected tt- bkg. 0.4 ± 0.4 Expected qq bkg. 7.8 ± 0.3 Total expected bkg. 8.2 ± 0.5 Observed events 7 No evidence for signal ! Sensitivity signal region signal region < 4.2 × 10-7 @ 90% CL Branching ratio < 2.5 × 10-7 @ 90% CL Richard Kass TAU06 Sept 19 2006 13 Search for t- 3p- 2p+ 2p0nt Richard Kass TAU06 Sept 19 2006 14 t Background Estimate t- 3p- 2p+ 2p0nt t 5pp0nt Background After all cuts the t background is dominated by the t 5pp0nt mode. MC Generate a large sample (3x data) of MC events for t 5pp0nt Fit 5pp0 pseudo-mass with a ‘crystal ball’ PDF allowing hadrons on the tag side gives more statistics Use the shape parameters to fit the pseudo-mass after all cuts. 5pp0 MC Scale expected bkg. to 232 fb-1 MC Expected (fit): 3.6 ± 0.6 events Richard Kass MC Counted : 3.2 events Other MC t bkg. 0.7 ± 0.5 events TAU06 Sept 19 2006 15 qq Background Estimate t- 3p- 2p+ 2p0nt MC Fit qq with a double Gaussian (uu/dd/ss, cc). data – tMC = qqDATA Fit qqDATA above 1.8 GeV/c2 with qqMC PDF, allowing PDF shape parameters float Extrapolate the fit below 1.8 GeV/c2 BABAR Data Expected (fit): 2.2 1.7 -1.0 MC PDF Data PDF events blinded Validate method by requiring at least three high energy photons on the tag side. Signal efficiency <0.01% Richard Kass TAU06 Sept 19 2006 16 qq bkgd. t bkgd. Signal Efficiency t- 3p- 2p+ 2p0nt Systematic Error Estimate Richard Kass Tracking efficiency Reconstruction of 2p0 Single photon Particle ID Limited MC statistics 3.9 % 6.6 % 1.8 % 1.7 % 1.8 % Total uncertainty of signal efficiency (%) 8.3 % Tracking, Neutrals, PID, p0 BR (t 5pp0nt) Fitting 8.4 % 14.9 % 16.7 % t 5pp0nt background t 3p2p0nt background Total t background 3.6 ± 0.9 events 0.7 ± 0.5 events 4.3 ± 1.0 events 1 .6 -1 .0 0 .7 - 0 .0 PDF parameters Fit function events events Total qq background 2.2 -11..07 events Luminosity and tt- cross-section 2.3 % TAU06 Sept 19 2006 17 t- 3p- 2p+ 2p0nt Results BABAR Signal eff. 0.66 ± 0.05 % 2 .0 Total expected bkg. 6.5 -1.4 Observed events 10 No evidence for signal ! Sensitivity < 1.8 × 10-6 @ 90% CL Branching ratio < 3.4 × 10-6 @ 90% CL Calculated using Cousins-Highland approach incorporating errors R. Barlow, Comput. Phys. Commun. 149, 97 (2002) Richard Kass TAU06 Sept 19 2006 18 Search for t- 2ωp-nt Motivation t 2wpnt should dominate the t 5p 2p0nt Pre-selection decay mode (PRD 60, 017301 (1999)) Kinematic constraints of t 2wpnt suppress the bkg. and allows to loosen the cuts. BABAR Sensitivity of O(10-7) can be achieved. Omega Reconstruction Loosen photon and p0 selection criteria w peak Allow hadrons on the tag side BABAR Significantly relax bkg. suppression cuts. Require 0.76 < Mp+p-p0 < 0.80 GeV/c2 2w efficiency: 8.2% 2w purity: Richard Kass 87% TAU06 Sept 19 2006 19 t- 2ωp-nt Results Kinematics of this decay greatly suppresses the background BABAR Only contribution is from the t w3pnt Signal eff. 1.53 ± 0.13 % Total exp. bkg. 0.4 -10..04 τ background Observed events 1 No evidence for signal ! Sensitivity < 4.3 × 10-7 @ 90% CL BR (t- 2w p- nt ) < 5.4 × 10-7 @ 90% CL Richard Kass TAU06 Sept 19 2006 20 Summary and Conclusions Multi-pion mode t 7p (p0)nt Previous BABAR < 2.4 × 10-6 < 3.0 × 10-7 t 7p nt N/A < 4.3 × 10-7 PRD72:012003, 2005 t 7p p0 nt N/A < 2.5 × 10-7 t 5p 2p0nt < 1.1 × 10-4 < 3.4 × 10-6 t 2w pnt N/A < 5.4 × 10-7 PRD74:011103, 2006 More details: “Search for Rare Multi-Pion Decays of the Tau Lepton Using the BABAR Detector” PhD thesis, Ruben Ter-Antonyan, Ohio State University, 2006. Tau decays to 7 or more particles (+ neutrino) have not been observed yet. Unlikely to be observed with < 1 ab-1 of data Challenge to theory/theorists to predict these decay rates Richard Kass TAU06 Sept 19 2006 21 Backup Slides Richard Kass TAU06 Sept 19 2006 22 PEPII-Asymmetric e+e- Collider Stanford Linear Accelerator Center, Stanford, California SLAC is an asymmetric e+e− collider: 9 GeV (e-)/3.1 GeV (e+) Center of Mass has bg=0.56 Richard Kass TAU06 Sept 19 2006 23 The BABAR Detector Electromagnetic Calorimeter (EMC) 1.5 T Solenoid Detector of Internally Recflected Cherenkov Light (DIRC) Drift Chamber (DCH) Instrumented Flux Return (IFR) Silicon Vertex Tracker (SVT) BABAR features: Charged particle tracking (silicon+drift chambers+1.5T Bfield) Electromagnetic calorimetry (CsI) g and electron ID p/K/p separation up to the kinematic limit (dE/dx+DIRC) Muon/KL identification Richard Kass TAU06 Sept 19 2006 24 Pseudo-mass Data-MC Comparison t- 3p- 2p+ 2p0nt t- 4p- 3p+ (p0) nt Pseudo-mass shapes of qq data and MC in agreement Gaussian function is a good fit To estimate qq bkg. in signal region, fit data with a PDF extracted from MC Richard Kass TAU06 Sept 19 2006 25 Bayesian Approach P( | x) = L( x | ) P( ) L( x | ' ) P( ' )d ' Bayes’ theorem P( | x) - probability of unknown given observed vector of data x L( x | ) - likelihood function for the data x given a certain up 1- = low P( | x)d - fraction of probability in a given interval [up, low] ( s b) n -( s b ) - likelihood for Poisson distributed n observed events L( n | s ) = e with expected background b, and a certain signal s n! 1 - = P( s | n)ds = sup - sup - - L(n | s) P( s)ds L(n | s) P( s)ds sup – upper limit at confidence level 1- Particle Data Group 2004 Richard Kass TAU06 Sept 19 2006 26 Bayesian Approach In our case, we want the upper limit on the branching ration: m -b B= 2 Ntt m = <n> is the mean of the number of observed events (Poisson) b – number of expected background with error sb (Gaussian) 2Ntt = f – scale factor with error sf (Gaussian) Likelihood vs. BR Maximize the likelihood wrt. f, b to obtain B: B(t- 4p- 3p+ (p0) nt ) = 0.7 -11..34 10 -7 Integrate over all permitted values of f and b to obtain the likelihood function in the branching fraction: B(t- 4p- 3p+ (p0) nt ) < 3.0 × 10-7 @ 90%CL Richard Kass TAU06 Sept 19 2006 BR 27 t- 4p- 3p+ (p0) nt Consistency Check DATA t bkg. qq bkg. Observed Topology 128 13 574 21 695 Particle ID 28 6 241 10 244 Conv. Veto 2.4 1.3 119 5 104 1-prong Tag 1.3 1.0 20.3 0.8 24 Cuts Richard Kass Cuts free fit fixed fit Topology 574 21 574 21 Particle ID 222 19 241 10 Conv. Veto 126 18 119 5 1-prong Tag 20.2 7.7 20.3 0.8 TAU06 Sept 19 2006 Agreement between exp. and obs. is consistent throughout cuts Agreement between fixed and free fits is consistent throughout cuts 28 t- 3p- 2p+ p0nt Background Error Estimate s s Generate Toy MC for 2D gaussian of m and s (fit parameters) and their errors. Correlation between m and s is taken into account. Using accept/reject method, plot the estimated bkg. for accepted toy MC fit parameters. ± 1s from the central value is the error. Richard Kass TAU06 Sept 19 2006 29 qq Background Validation t- 3p- 2p+ 2p0nt Require ≥3 high-energy (Eg > 300 MeV) photons on 1-pr. side, not associated with p0 Signal efficiency <0.01% Suppresses tau events, leaving clean qq sample in the data, which can be studied unblinded t 5p2p0nt BABAR Data fit of the qq pseudo-mass spectrum with a PDF taken from MC nicely describes the tail of the spectrum and gives a valid estimate of expected bkg. events in the signal region Observe: 12 events Predict: 11.8 events Richard Kass TAU06 Sept 19 2006 30 t- 2ωp-nt Background Estimate blinded blinded blinded blinded t bkg. qq bkg. generic t: 0 events 1.0 t w3pnt: 0.4 - 0.4 events Poisson err. 68% CL pseudo mass shapes of data and scaled MC agree no tail expected due to kinematical constraints extrapolation expected qq bkg: 0 0.1 -0 Richard Kass TAU06 Sept 19 2006 31 Measurement of BR(t5p p0nt) as a Cross Check BABAR Preliminary Repeat the event selection of t5p 2p0nt (reconst. 1 p0) Total bkg. Repeat the background estimate method. Validate qq bkg. estimate with ‘signal-free’ data sample (≥3 high-energy photons on the tag side) Signal efficiency (%) 2.16 ± 0.16 % Expected tau bkg. 67 ± ZZ Expected qq bkg. 84 ± YY ALEPH, 96 1.8 ± 0.7 ± 1.2 Observed Data 1742 OPAL, 99 2.7 ± 1.8 ± 0.9 Observed Signal 1591 ± XX ±XX CLEO, 01 1.7 ± 0.2 ± 0.2 PDG, 04 1.81 ± 0.27 Branching Ratio (x10-4) BR(t5pp0nt) 1.79 ± XXX ± XXX Nice cross-check of the event selection and background estimate methods Richard Kass TAU06 Sept 19 2006 32