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Insertion of STC into TRT at the Department of Physics, Oxford
Credit: CERN

Sneha Malde

Associate Professor of Physics

Sub department

  • Particle Physics

Research groups

  • LHCb
Sneha.Malde@physics.ox.ac.uk
Telephone: 01865 (2)73357
Denys Wilkinson Building, room 673
  • About
  • Publications

First observation of the decay B(s)^0 → K(S)^0K∗(892)^0 at LHCb

Journal of High Energy Physics Springer Verlag 2016:12 (2016)

Authors:

R Aaij, B Adeva, M Adinolfi, Neville Harnew

Abstract:

First observation of the decay Bs0 → KS0K∗(892)0 at LHCb

A search for B(s)0 → KS0K∗(892)0 decays is performed using pp collision data, corresponding to an integrated luminosity of 1.0 fb−1, collected with the LHCb detector at a centre-of-mass energy of 7 TeV. The Bs0 → KS0K∗(892)0 decay is observed for the first time, with a significance of 7.1 standard deviations. The branching fraction is measured to be
𝓑(Bs0 → K̅0K∗(892)0) + 𝓑(Bs0 → K0K̅∗(892)0)=(16.4 ± 3.4 ± 2.3) × 10−6,
where the first uncertainty is statistical and the second is systematic. No evidence is found for the decay B0 → KS0K∗(892)0 and an upper limit is set on the branching fraction, 𝓑(B0 → K̅0K∗(892)0) + 𝓑(B0 → K0K̅∗(892)0) < 0.96 × 10−6, at 90 % confidence level. All results are consistent with Standard Model predictions.

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Amplitude analysis of B−→D+π−π− decays

Physical Review D American Physical Society 94:7 (2016) 072001

Authors:

Shu-Faye Cheung, Tim Evans, Paolo Gandini, Barak R Gruberg Cazon, Thomas Hadavizadeh, Neville Harnew, D Hill, N Hussain, Pawel Jalocha, Malcolm JJ John, Oliver S Lupton, Sneha S Malde, Anita K Nandi, W Qian, S Stevenson, C Thomas, Stig Topp-Joergenson, Guy R Wilkinson

Abstract:

The Dalitz plot analysis technique is used to study the resonant substructures of B−→D+π−π− decays in a data sample corresponding to 3.0  fb−1 of pp collision data recorded by the LHCb experiment during 2011 and 2012. A model-independent analysis of the angular moments demonstrates the presence of resonances with spins 1, 2 and 3 at high D+π− mass. The data are fitted with an amplitude model composed of a quasi-model-independent function to describe the D+π− S wave together with virtual contributions from the D∗(2007)0 and B*0 states, and components corresponding to the D∗2(2460)0, D∗1(2680)0, D∗3(2760)0 and D∗2(3000)0 resonances. The masses and widths of these resonances are determined together with the branching fractions for their production in B−→D+π−π− decays. The D+π− S wave has phase motion consistent with that expected due to the presence of the D∗0(2400)0 state. These results constitute the first observations of the D∗3(2760)0 and D∗2(3000)0 resonances, with significances of 10σ and 6.6σ, respectively.
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Measurement of the CKM angle γ using B0 → DK*0 with D → KS0π+π− decays

Journal of High Energy Physics Springer Berlin Heidelberg 2016:8 (2016)

Abstract:

A model-dependent amplitude analysis of the decay B0 → D(KS0π+π−)K∗0 is performed using proton-proton collision data corresponding to an integrated luminosity of 3.0 fb−1, recorded at √s=7 and 8 TeV by the LHCb experiment. The CP violation observables x± and y±, sensitive to the CKM angle γ, are measured to bex−=−0.15±0.14±0.03±0.01,y−=0.25±0.15±0.06±0.01,x+=0.05±0.24±0.04±0.01,y+=−0.65−0.23+0.24±0.08±0.01, where the first uncertainties are statistical, the second systematic and the third arise from the uncertainty on the D → KS0π+π− amplitude model. These are the most precise measurements of these observables. They correspond to γ = (80−22+21)° and rB0=0.39±0.13, where rB0 is the magnitude of the ratio of the suppressed and favoured B0 → DK+π− decay amplitudes, in a Kπ mass region of ±50 MeV around the K*(892)0 mass and for an absolute value of the cosine of the K*0 decay angle larger than 0.4.[Figure not available: see fulltext.]
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Observation of Bs0 → D 0 KS0 and Evidence for Bs0 → D ∗0 KS0 Decays

Physical Review Letters American Physical Society 116:16 (2016) 161802

Authors:

R Aaij, S-F Cheung, T Evans, P Gandini, R Gauld, E Greening, T Hadavizadeh, Neville Harnew, D Hill, N Hussain, J Jalocha, M John, O Lupton, S Malde, A Nandi, E Smith, S Stevenson, C Thomas, S Topp-Joergensen, N Torr, G Wilkinson

Abstract:

The first observation of the Bs0→D0KS0 decay mode and evidence for the Bs0→D∗0KS0 decay mode are reported. The data sample corresponds to an integrated luminosity of 3.0 fb-1 collected in pp collisions by LHCb at center-of-mass energies of 7 and 8 TeV. The branching fractions are measured to be B(Bs0→D0K0)=[4.3±0.5(stat)±0.3(syst)±0.3(frag)±0.6(norm)]×10-4,B(Bs0→D∗0K0)=[2.8±1.0(stat)±0.3(syst)±0.2(frag)±0.4(norm)]×10-4,where the uncertainties are due to contributions coming from statistical precision, systematic effects, and the precision of two external inputs, the ratio fs/fd and the branching fraction of B0→D0KS0, which is used as a calibration channel.
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Quantum-correlated measurements of D0 → KS0π+π−π0 and consequences for the determination of γ

Proceedings of Science 2016-November (2016)

Authors:

PK Resmi, J Libby, S Malde, G Wilkinson

Abstract:

Quantum-correlated measurements of the decay D0 → KS0π+π−π0 are performed with a data sample corresponding to an integrated luminosity of 818 pb−1 collected at the ψ(3770) resonance by the CLEO-c detector. Preliminary results are presented for the CP-even fraction F+ and the strong-phase differences of this decay. The value of F+ is measured to be 0.246 ± 0.018. The strong-phase differences are measured in different regions of KS0π+π−π0 phase space by binning around the intermediate resonances present. The potential sensitivity of the results for determining the CKM angle γ from B± → D(KS0π+π−π0)K± decays using data collected by the Belle detector is also shown.

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