B D ( ) τν τ decays with hadronic and semileptonic tagging at Belle

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1 B D ( ) τν τ decays with hadronic and semileptonic tagging at Belle Pablo Goldenzweig KIT Moriond EW La Thuile, Italy March 12-19, 2016

2 Outline Review of Belle s 2015 result of B D ( ) τ ν τ with hadronic tagging, and the current world average. Introduce Belle s new measurement of B 0 D + τ ν τ with the semileptonic tagging method and compatibility with New Physics models. P. Goldenzweig B D ( ) τν τ at Belle / 19

3 The Belle Experiment The Belle detector The KEKB accelerator Asymmetric e+ e collider Mainly operates at the Υ(4S) resonance Final data sample 711f b 1 Υ(4S) resonance 121f b 1 Υ(5S) resonance P. Goldenzweig B D ( ) τ ν τ at Belle / 19

4 B D ( ) τν decays and 2HDM Semitauonic B decays of type b cτ ν τ are sensitive probes to search for New Physics. NP could change B and τ polarization. Effect could be different for D and D. 2HDM of type II A charged Higgs of spin 0 couples to the τ. Could enhance or decrease the ratios R(D ( ) ) = B(B D( ) τ ν) B(B D ( ) lν) depending on tan 2 β/m 2 H ±. BaBar 2013: The combination of R(D) and R(D ) excludes the type II 2HDM charged Higgs boson at 99.8% confidence level for any value of tan β/m H ±. Phys. Rev. D (2013) P. Goldenzweig B D ( ) τν τ at Belle / 19

5 Principle of the measurement Measure the ratios: R(D ( ) ) = B(B D( ) τ ν) B(B D ( ) lν) = signal normalization (l = e, µ) τ reconstructed only using leptonic decays, τ lν τ ν l : Signal and normalization are identified by the same particles in the final state. Leads to cancellation of dependence on form factors, the CKM matrix element V cb, and on various sources of uncertainty in the ratios R(D ( ) ). Also allows for precise SM predictions with uncertainties 2% (6%) for R(D) (R(D )). Phys. Rev. D 78, (2008), Phys. Rev. D 85, (2012) Experimentally challenging: Neutrinos in the final state prohibit direct signal-side reconstruction Must fully reconstruct e + e Υ(4S) B tag B sig events P. Goldenzweig B D ( ) τν τ at Belle / 19

6 The Full Reconstruction method Typical B factory event K + π + π e π π + t t Tag- and signal-side of the full reconstruction 1 2 t 3 t 4 tag side signal side t 5 Hierarchical reconstruction of the B tag using NeuroBayes 1. Check if the remaining particles in the detector are consistent with the signal signature. 1 Nucl. Instrum. Meth. A654: 432 (2011) P. Goldenzweig B D ( ) τν τ at Belle / 19

7 Which tag-side reconstruction? Tagging techniques Purity Efficiency Inclusive B anything ɛ O(2%) Very large statistics; Also very large background Semileptonic B D ( ) lν l ɛ O(0.2%) Mid-range reconstruction efficiency; Less information about B tag due to neutrino Hadronic B hadrons ɛ O(0.1%) Cleaner sample Knowledge of p(b sig ); Lower tagging efficiency P. Goldenzweig B D ( ) τν τ at Belle / 19

8 Belle hadronic tag result (2015) Phys. Rev. D 92, R(D) = ± ± R(D ) = ± ± Fit is repeated with PDF generated for type II 2HDM with tanβ/m H = 0.5 GeV 1 Belle result lies between the SM prediction (1.4σ away) and BaBar s hadronic tag result (1.8σ away) Phys. Rev. D 88, (2013) Compatible with type II 2HDM around tanβ/m H = 0.5 GeV 1 P. Goldenzweig B D ( ) τν τ at Belle / 19

9 Including LHCb R(D ) measurement R(D*) BaBar, PRL109,101802(2012) Belle, arxiv: LHCb, arxiv: Average 2 χ = SM prediction HFAG Prel. EPS2015 P(χ 2 ) = 55% R(D) 3.9σ combined deviation (including correlations) from the SM P. Goldenzweig B D ( ) τν τ at Belle / 19

10 New measurement of R(D ) with SL tag Semitauonic signal-side decay and semileptonic tag-side. Normalization events are double semileptonic decays. Numerator in R(D ) Denominator in R(D ) D reconstruction: D + D 0 π +, D + π 0 ( 100%) D 0 : 10 modes ( 37%) D + : 5 modes ( 22%) Tag semileptonic B-decay: Combine D + and oppositely-charged lepton candidates and calculate the cosine of the angle between the B momentum and the D l in the Υ(4S) frame. tag candidates: cos θ B-D l [ 1, 1] Image credits: Y. Sato (Nagoya) P. Goldenzweig B D ( ) τν τ at Belle / 19

11 Determination of R(D ) Separate correctly reconstructed signal and normalization events using NeuroBayes NN with the following variables: Missing mass squared: M 2 miss = (2E beam i Ei)2 i pi 2 Visible energy: E vis = i Ei, where ( pi, Ei) is the reconstructed fourmomentum at the Υ(4S) rest frame of particles used in the reconstruction. cos θ B-D l Trained on MC samples of signal and normalization. Dominant backgrounds: Fake (falsely reco d) D. B D lν l, with D D ( ) B X cd, with X c decaying semileptonically. Separated from signal and normalization using the sum of energies of neutral clusters not associated with reco d particles: E ECL 2D fit to NN and E ECL to extract signal and normalization Component Yield Shape Signal Float 1D X 1D Normalization Float 2D Fake D ( ) Fix 2D B D lν Float 2D Other Fix 2D P. Goldenzweig B D ( ) τν τ at Belle / 19

12 Determination of R(D ) 2D fit to NN and E ECL : Preliminary R(D ) = 1 B(τ l ν l ν τ ) εnorm ε sig N sig N norm ε norm /ε sig = ± (from MC simulation) R(D ) = ± 0.030(stat) ± 0.011(syst) (13.8σ) P. Goldenzweig B D ( ) τν τ at Belle / 19

13 Systematic uncertainties and cross-checks R(D ) [%] Sources l sig = e, µ l sig = e l sig = µ MC statistics for PDF shape 2.2% 2.5% 3.9% +1.1 PDF shape of the normalization 0.0 % % % PDF shape of B D +1.0 lν l 1.7 % % % PDF shape and yields of fake D ( ) 1.4% 1.6% 1.6% PDF shape and yields of B X cd 1.1% 1.2% 1.1% Reconstruction efficiency ratio ε norm/ε sig 1.2% 1.5% 1.9% Modeling of semileptonic decay 0.2% 0.2% 0.3% B(τ l ν l ν τ ) 0.2% 0.2% 0.2% Total systematic uncertainties % % % Dominant uncertainty arises from the limited size of the MC samples for the PDF shapes. Evaluated with Toy MC studies. Large error due to poorly known B(B D lν l ) and of the D decay. Varied within their uncertainties. Consistent results for individual samples B sig) R(D ) = ± ± (l sig = e) R(D ) = ± ± (l sig = µ) P. Goldenzweig B D ( ) τν τ at Belle / 19

14 Comparison with other measurements Preliminary Central value close to Belle hadronic tag result. Precision improvement over Belle hadronic tag and LHCb results. P. Goldenzweig B D ( ) τν τ at Belle / 19

15 Compatibility test at SM Kinematic variables: Preliminary The momentum transfer q 2 (p B p D ( )) 2 cannot be calculated with a semileptonic tag due to a neutrino on the tag side (employed in the hadronic analyses). Use the background-subtracted momenta of D and lepton in the CM frame in the signal region: NN > 0.8 and E ECL < Measured Expected 30 χ 2 /ndf = 20.3/19, p = 37.6 % 30 χ 2 /ndf = 21.4/18, p = 25.8 % p D * [GeV/c] p [GeV/c] l P. Goldenzweig B D ( ) τν τ at Belle / 19

16 R(D ) in 2HDM type-ii Compatibility test: Preliminary 1) Construct a PDF for signal events for a scan of tan β/m H ± [0, 1]GeV 1. 2) Find that the measured value of R(D ) matches the theoretical prediction at tan β m H ± 0.7 GeV 1. 3) P -values of p D and p l similar to SM case. 30 χ 2 /ndf = 20.3/19, p = 37.9 % 30 R(D*) χ 2 /ndf = 22.2/18, p = 22.5 % Measured R(D*) (±1σ) Theory tanβ/m H+ [GeV ] p D * [GeV/c] p [GeV/c] l P. Goldenzweig B D ( ) τν τ at Belle / 19

17 B D ( ) τν τ decays and Leptoquarks Bosons which couple to a lepton-quark pair. Carry color & electric charge, baryon &lepton #. Unified description of leptons and quarks. Six LQ Models Scalar Vector 6 LQ models in b cτ ν τ decays B D ( ) τ ν is sensitive to the tensor operator. R 2 -type LQ model good candidate for compatibility test. Relative Wilson coeffs. C S2 = +7.8 C T at the b mass scale, assuming M LQ = O(1) TeV. References: PRD 87, (2013); PRD 88, (2013). Image credits: Y. Sakaki (KEK) P. Goldenzweig B D ( ) τν τ at Belle / 19

18 R(D ) in R 2 -type Leptoquark Compatibility test: Preliminary R(D*) 0.6 Theory Two favored regions found: C T = 0.03 C T = (shown below) Large disagreement in D momentum distribution ~SM Measured R(D*) (±1σ) SM χ 2 /ndf = 35.1/19, p = 1.4 % 30 χ 2 /ndf = 23.8/18, p = 16.2 % C T p D * [GeV/c] p [GeV/c] l P. Goldenzweig B D ( ) τν τ at Belle / 19

19 Summary B D ( ) τ ν τ results with hadronic tag compatible with type II 2HDM around tanβ/m H = 0.5 GeV 1. First result of B 0 D + τ ν τ with the semileptonic tagging method shown today. Central value close to Belle hadronic tag result. Precision improvement over Belle hadronic tag and LHCb results. Compatible with the SM and type-ii 2HDM around tanβ/m H = 0.7 GeV 1. R 2 type leptoquark model with C T = is disfavored. To be submitted to PRD this month. P. Goldenzweig B D ( ) τν τ at Belle / 19