Time-dependent CPV in B η'ks η

Size: px
Start display at page:

Download "Time-dependent CPV in B η'ks η"

Transcription

1 B ± ωk ω ± /π ± and Time-dependen CPV in B η'ks η a Belle Kai-Feng Chen Naional Taiwan Universiy The Belle Collaboraion Flavor Physics & CP Violaion(FPCP) Universiy of Pennsylvania, Philadelphia May 16-18, Inroducion B ± ωk ± CP in B η'ks Summary

2 Inoducion Rare B decays are useful o deermine he uniary riangle. Tes of curren undersanding of B physics. Search for CP violaion and probe new physics. B π l ν B D S π V ud V * ub B ππ B ρπ φ (α) B-B mixing V d V * b φ 3 (γ) B DK B ππ/kπ B ωk Oher charmless B decays V cd V * cb B D(*) l ν φ 1 (β) B J/ψK B D(*)D(*) B η'k

3 B ± ωh ± Inroducion b B u b B u W W u,c, g u d, s u u s u u u π, K ω K ω B ± ωh ± can es B decay models. Useful o search for direc CP violaion. Brief Hisory: CLEO firs repored he B ± ωk ± decay branching fracions in [PRL 81, 7(1998)] B ± ωπ ± is found o be larger han ωk ± wih new daa se. [PRL 8, 881()] BaBar confirms B ± ωπ ± >ωk ±. [PRL 87, 18(1)] (B ωπ)x1-6 (B ωκ)x1-6 7 CLEO(1998) < CLEO().9 1. < BaBar(1) < 1..3

4 B ± ωh ± Resuls Resuls from 31.9M BB pairs. Yields are exraced by a -dimensional unbinned likelihood mehod. Background from B decays Enries / MeV Enries / MeV E (GeV) 7.. Enries / MeV Enries / MeV Mb (GeV) Preliminary B ± ωk ± B ± ωπ ± E (GeV) Mb (GeV) Yield Σ ε B(x1-6 ) U.L B ωπ σ 7.7% 1.8. <8. B ωκ σ 6.3%. 1. -

5 Consisency Checks ωmass Evens / MeV Evens / MeV ω mass (GeV) 1 1 (a) (c) B ωk B ωπ (b) (d) coshel (a) A clear ω peak shown in π + π π specrum wih B candidae. (b) The ω heliciy angle disribuion maches P VP decay. (c),(d) By removing he KID requiremen, he E disribuion is consisen wih ωk and ωπ yields de (GeV) kid vs E

6 Direc CPV in B ± ωk ± Search for Acp in B ± ωk ± mode. K Acp(= ) = -.±.7±. K K 9% C.L.) K Enries / MeV Enries / MeV 3 1 B ωk - 7.±3. evens Enries / MeV ωk E (GeV) - Enries / MeV ωk Mb (GeV) - 6 Preliminary B ωk ±3.7 evens ωk E (GeV) ωk Mb (GeV) +

7 1. 3. Summary of B ± ωh ± We have observed B ± ωk ±, and evidence for B ± ωπ ± (ωk ± ) = (9.9 ±1.) x 1-6 (6.σ) (ωπ ± ) = (.3 ±.) x 1-6 (3.3σ) < 8. x 1-6 Compare resuls wih oher experimens: (B ωπ)x1-6 (B ωκ)x Belle() < BaBar(1) < CLEO() <8.8 Acp(ωK ± ) = -.±.7±. 9% C.L.).9 1.9

8 A S CPV in B η'k Wihin he SM, B η'k consiss of penguin process and conribuion from ree diagrams...,ec. The ime-dependen CP asymmery can be expressed as: A CP B B B B cos m S sin m sin m sin 1 NP sin m ( If A = )

9 Time-dependen Measuremen B B Ks η' daughers cp-side B B B B z = βγc l K ag-side/mdlh mehod B B X l X l, XD D, XD D YK YK,...,... Fully reconsruc B η'ks as cp-side.(η'k ± as conrol sample) The b-flavor is deermined by he accompanying B meson(bag) by a muli-dimensional likelihood mehod(mdlh). Deermine he CP parameers from he disribuion by an unbinned likelihood fi.

10 B η'k Reconsrucion Daa se for his analysis is fb -1. Two sub decay modes of η' are reconsruced: η' ηππ and η' ργ. A unbinned -dimensional likelihood fi is performed. Enries η'k + η'ks GeV E GeV/C Preliminary Mb η' ηππ Combined expeced BB background N(ηππ K + ) = 78. N(ργ K + )= 1 ±1 N(ηππ Ks)= 7. N(ργ Ks) =

11 Consisency Checks Checks by B-lifeime fi wih 9 η'k ± and 73 η'ks evens: BB + qq coninuum BB only B ± B ps z(rec)/(βγ) Ψ C CP-fi wih non-asymmeric sample: η'k ± ps z(rec)/(βγ) Ψ C Enries/ps τ(b ± ) = ps (PDG: 1.63±.8 ps) +.31 τ(b ) = ps (PDG: 1.8±.3 ps) q = +1 q = - 1 sin(φ 1 +φ NP ) = S(η'K ± ) =.11±.9 A(η'K ± ) = -.7± ps (ps) Asymmery ± 1σ error

12 Time-dependen Acp CP-fi is performed wih 73 η'ks signal candidaes. Enries/ps 1 (a) q = +1 S(η'Ks) = A(η'Ks) =.1±.3 3 (b) q = - 1 If A(η'Ks) is se o be zero: +.3 sin(φ 1 +φ NP ) =.9 -. Firs measuremen of imedependen CPV in B η'ks decay. Probe phases from New Physics. 1 1 (c) q = +1 q = (d) η K S ± 1σ error ps Asymmery (ps) Preliminary

13 Sysemaic Uncerainies Sysemaic uncerainies are deermined by repeaing fi on daa wih ±1σ o each parameers. Sysemaic uncerainies include S(η'Ks) A(η'Ks) sin(φ1+φ NP ) Verexing/rack selecion +./ /-.3 +./-. Physics parameers +.3/ /-. +./-.3 Wag fracions +.3/ / /-. Resoluion funcion +./ /-.1 +./-.3 PDF funcions +.3/ /-. +./-. Even fracions +./-. +.1/-.1 +./-. BB background +./-. +./-.1 +./-.1 Sum +.7/ / /-.7 Preliminary

14 Summary of CPV in η'k Firs measuremen of ime-dependen CPV parameers in B η'ks decay Probe for phases from New Physics S(η'Ks) =.7 (sa.) ±.7(sys.) A(η'Ks) =.1 ±.3(sa.) ±.7(sys.) If A(η'Ks) se o be zero: +.3 sin(φ 1 +φ NP ) =.9 -. (sa.) ±.7(sys.) Belle sin(φ 1 ) =.8 ±.1(sa.) ±.(sys.) Preliminary

15 Conclusion B ± ωh ± We have observed B ωk ± Evidence for B ωπ ±. Firs look a direc CPV in B ωk ±. CP in B η'k Firs measuremen of imedependen CPV in B η'ks decay. Perspecives More daa are coming soon 8 fb -1 per monh. 9fb -1 for summer ±.3 for 9fb -1 saisical error ±.1 for 3fb fb-1 Saisical Error VS. Luminosiy

Rare Hadronic B Decays

Rare Hadronic B Decays XLI st Rencontres de Moriond QCD and High-Energy Hadronic Interactions La Thuile, Italy, March 18-5, 6 Rare Hadronic B Decays Jürgen Kroseberg Santa Cruz Institute for Particle Physics University of California,

More information

Rare Hadronic B decays at BaBar

Rare Hadronic B decays at BaBar Rare Hadronic B decays at BaBar Mirna van Hoek University of Colorado On behalf of the BaBar Collaboration 18 th International Workshop on Weak Interactions and Neutrinos January 21-26, 2002 Christchurch,

More information

Multivariate analysis of H b b in associated production of H with t t-pair using full simulation of ATLAS detector

Multivariate analysis of H b b in associated production of H with t t-pair using full simulation of ATLAS detector Mulivariae analysis of H b b in associaed producion of H wih -pair using full simulaion of ATLAS deecor Sergey Koov MPI für Physik, München ATLAS-D Top meeing, May 19, 26 Sergey Koov (MPI für Physik, München)

More information

Results on B decays from BaBar

Results on B decays from BaBar Results on B decays from BaBar Vasilii Shelkov Lawrence Berkeley National Laboratory BaBar Collaboration 1 The BaBar Collaboration 2 9 Countries, 72 Institutions, 554 Physicists 3 Instrumented Flux Return

More information

TOP-QUARK MASS MEASUREMENTS AT THE LHC

TOP-QUARK MASS MEASUREMENTS AT THE LHC TOP-QUARK MASS MEASUREMENTS AT THE LHC S. Blyweer, on behalf of he ATLAS and CMS Collaboraions Vrije Universiei Brussel - Ineruniversiy Insiue for High Energies Pleinlaan 2, 1050 Brussel, Belgium The op-quark

More information

A SSOCIATED TOP PRODUCTION (tt +V, t +V ) IN ATLAS AND CMS

A SSOCIATED TOP PRODUCTION (tt +V, t +V ) IN ATLAS AND CMS S ERGIO S ANCHEZ C RUZ FOR THE ATLAS AND CMS C OLLABORATIONS Renconres de Moriond 08 A SSOCIATED TOP PRODUCTION ( +V, +V ) IN ATLAS AND CMS σ [pb] Producion Cross Secion, 3 Sepember 07 =n je(s) CMS Preliminary

More information

Top Quark Mass Measurements at the Tevatron. Gianluca Petrillo (for the CDF and DØ collaborations) University of Rochester

Top Quark Mass Measurements at the Tevatron. Gianluca Petrillo (for the CDF and DØ collaborations) University of Rochester Top Quark Mass Measuremens a he Tevaron Gianluca Perillo (for he CDF and DØ collaboraions) Universiy of Rocheser March 13 h, 013, Renconres de Moriond: QCD and High Energy Ineracions CDF G. Perillo (for

More information

B. Hoeneisen. Universidad San Francisco de Quito Representing the DØ Collaboration Flavor Physics and CP violation (2013)

B. Hoeneisen. Universidad San Francisco de Quito Representing the DØ Collaboration Flavor Physics and CP violation (2013) Status report on the like-sign dimuon charge asymmetry in p p collisions and Measurement of the direct CP asymmetry in B J/ψK and B J/ψπ decays B. Hoeneisen Universidad San Francisco de Quito Representing

More information

The other window on New Physics: CP violation at the B factories

The other window on New Physics: CP violation at the B factories The other window on New Physics: CP violation at the B factories Gabriella Sciolla M.I.T. Outline: The physics of CP violation What is CP and why is it interesting? CPV in the B system CPV in the Standard

More information

Heavy Quarks and τ. CVC test Michel parameters. Charm Mixing f D s

Heavy Quarks and τ. CVC test Michel parameters. Charm Mixing f D s Heavy Quarks and τ University of Illinois CVC test Michel parameters Charm Mixing f D s B f B Two mysteries: N c and η K CKM: ππ, Kπ, V cb, V ub Lifetime and mixing CP search Belle and Babar* A very brief

More information

HIGGS&AT&HADRON&COLLIDER

HIGGS&AT&HADRON&COLLIDER IGGS&AT&ADRON&COLLIDER iggs&proper,es&and&precision&tes& Lecure&1& Shahram&Rahalou Fisica&delle&Par,celle&Elemenari,&Anno&Accademico&014815 hp://www.roma1.infn.i/people/rahalou/paricelle/ WY&AND&WIC&BOSON?

More information

Measurements of CP violating phases in B decays at LHCb

Measurements of CP violating phases in B decays at LHCb Measurements of CP violating phases in B decays at Sevda Esen [Heidelberg University] on behalf of the collaboration Les Rencontres de Physique de la Vallée d Aoste, 1-7 March 215 CP Violation in the SM

More information

Measurement of ϕ 2 /α using

Measurement of ϕ 2 /α using Measurement of ϕ 2 /α using Decays at elle and aar lexander Somov CKM 6, Nagoya 26 Introduction (CP violation in decays Measurements in φ 2 constraint from an Isospin analysis CP Violation in decays Tree

More information

Recent Results on Rare B Decays from BaBar and Belle

Recent Results on Rare B Decays from BaBar and Belle SLACPUB-97 April 3 1 Recent Results on Rare B Decays from BaBar and Belle B. Brau a, a Laboratory for Nuclear Science, Massachusetts Institute of Technology 77 Massachusetts Avenue, Cambridge, MA, 2139

More information

Weak Decays, CKM, Anders Ryd Cornell University

Weak Decays, CKM, Anders Ryd Cornell University Weak Decays, CKM, CP Violation Anders Ryd Cornell University Presented at the International Conference on Weak Interactions and Neutrinos Delphi, Greece, June 6-11, 2005 Page: 1 Flavor Physics The study

More information

CP violation in B 0 π + π decays in the BABAR experiment. Muriel Pivk, CERN. 22 March 2004, Lausanne

CP violation in B 0 π + π decays in the BABAR experiment. Muriel Pivk, CERN. 22 March 2004, Lausanne CP violation in B π + π decays in the BABAR experiment, 22 March 24, The BABAR experiment at SLAC 2 Phenomenology 3 The h + h analysis 4 A new tool: s Plots 5 Results 6 Interpretation of the results 7

More information

Mikihiko Nakao (KEK) June 16th, 2006, SUSY06, Newport Beach, CA.

Mikihiko Nakao (KEK) June 16th, 2006, SUSY06, Newport Beach, CA. at BELLE and BABAR. Mikihiko Nakao (KEK) June 16th, 26, SUSY6, Newport Beach, CA mikihiko.nakao@kek.jp. Huge number of coherent / energy-asymmetric BB production at Y(4S) slow π e / µ K B or B (flavor

More information

Recent results on CKM/CPV from Belle

Recent results on CKM/CPV from Belle Recent results on CKM/CPV from Belle Alexander Leopold for the Belle Collaboration Insitute of High Energy Physics Austrian Academy of Sciences HEPMAD 15, September 21 st 2015 A. Leopold (HEPHY) Belle

More information

Flavour Physics at hadron machines

Flavour Physics at hadron machines Flavour Physics at hadron machines KIAS Phenomenology Workshop Seoul, Korea, 17-19 November 2011 T. Nakada EPFL-LPHE Lausanne, Switzerland B physics, started with hadron machine First discovery of b-quark

More information

CP Violation in the B system

CP Violation in the B system CP Violation in the B system Outline: Mixing induced CPV and B s mixing phase s Search for CPV in B s mixing Direct CPV in B DK and CKM phase Direct CPV in charmless B decays new Ulrich Uwer Heidelberg

More information

LHCb Physics and prospects. Stefano Perazzini On behalf of LHCb Collabora4on MENU nd June 2010

LHCb Physics and prospects. Stefano Perazzini On behalf of LHCb Collabora4on MENU nd June 2010 LHCb Physics and 2010-11 prospects Stefano Perazzini On behalf of LHCb Collabora4on MENU2010 2 nd June 2010 Physics: OUTLINE Flavor physics and CPV in the quark sector Search for New Physics The LHCb Experiment

More information

Hadronic Charm Decays: Experimental Review

Hadronic Charm Decays: Experimental Review Hadronic Charm Decays: Experimental Review Featuring results from Peter Onyisi ICHEP, 1 Aug 2008 Peter Onyisi Hadronic Charm Decays: Experimental Review ICHEP, 1 Aug 2008 1 What Can We Learn? Hadronic

More information

Charmless B Decays. Wolfgang Gradl For thebabar and BELLE collaborations. Heavy Quark and Leptons The University of Edinburgh I V E R S I T Y

Charmless B Decays. Wolfgang Gradl For thebabar and BELLE collaborations. Heavy Quark and Leptons The University of Edinburgh I V E R S I T Y Charmless B Decays Wolfgang Gradl For thebabar and BELLE collaborations The University of Edinburgh T H E U N I V E R S I T Y O H F E D I N B U R G Heavy Quark and Leptons 26 W. Gradl (U. Edinburgh) Charmless

More information

J PC =1 - - states spectroscopy, study of their decays Calculation of hadronic contributions into a µ and α QED (m Z )

J PC =1 - - states spectroscopy, study of their decays Calculation of hadronic contributions into a µ and α QED (m Z ) Study of e + e - a n n i h i l a ti on a t l ow e n e r g i e s Vladimir D ru z h in in Budker I n s t i t ut e o f N uc l ea r P h y s i c s ( N o v o s i b i rs k R us s i a ) S N D - Ba Ba r L ep t

More information

CLEO CLEO I.5 CLEO II CLEO II.V CLEO III

CLEO CLEO I.5 CLEO II CLEO II.V CLEO III CLEO CLEO I.5 CLEO II CLEO II.V CLEO III Recent Results on Beauty and Charm Klaus Honscheid Ohio State University SLAC Summer Institute 2000 SLAC Summer Institute Klaus Honscheid, Ohio State University

More information

CP Violation and Rare B Decays at Belle

CP Violation and Rare B Decays at Belle CP Violation and Rare B Decays at Belle DESY Seminar 11 Sep, 2001 M. Hazumi (Osaka University, Osaka, Japan) Representing the Belle Collaboration Outline Introduction KEKB Accelerator and Belle Detector

More information

G. Eigen U Bergen NFR Meeting Bergen October 19, 2005

G. Eigen U Bergen NFR Meeting Bergen October 19, 2005 G. Eigen U Bergen NFR Meeting Bergen October 19, 2005 Introduction The BABAR experiment was designed to measure sin 2 2 with high precision in the mode B J/ K 0 S For sin 2 2 no high precision results

More information

Measuring the Unitarity Triangle Angle α with BaBar. Adrian Bevan KEK, 15 th September 2006

Measuring the Unitarity Triangle Angle α with BaBar. Adrian Bevan KEK, 15 th September 2006 (C) Peter Ginter (2002). Measuring the Unitarity Triangle Angle α with BaBar Adrian Bevan KEK, 15 th September 2006 (α, β, γ) (φ 1, φ 2, φ 3 ) 15 th September 2006 Adrian Bevan 1 Overview Motivation PEP-II

More information

Evidence for D 0 - D 0 mixing. Marko Starič. J. Stefan Institute, Ljubljana, Slovenia. March XLII Rencontres de Moriond, La Thuile, Italy

Evidence for D 0 - D 0 mixing. Marko Starič. J. Stefan Institute, Ljubljana, Slovenia. March XLII Rencontres de Moriond, La Thuile, Italy Evidence for D - D mixing - D mixing (page 1) Introduction Mixing observed in K, Bd and B s (26), not yet in D system D mixing in the SM governed by box diagrams Effective GIM suppression mixing in D system

More information

11. The Top Quark and the Higgs Mechanism

11. The Top Quark and the Higgs Mechanism 11. The Top Quark and he Higgs Mechanism Paricle and Nuclear Physics Dr. Tina Poer Dr. Tina Poer 11. The Top Quark and he Higgs Mechanism 1 In his secion... Focus on he mos recen discoveries of fundamenal

More information

Flavor physics. Yuval Grossman. Cornell. Y. Grossman Flavor physics APS2009, Denver, 5/2/2009 p. 1

Flavor physics. Yuval Grossman. Cornell. Y. Grossman Flavor physics APS2009, Denver, 5/2/2009 p. 1 Flavor physics Yuval Grossman Cornell Y. Grossman Flavor physics APS2009, Denver, 5/2/2009 p. 1 Flavor at a junction Every end is a new beginning End: The Nobel to KM is a formal declaration that the CKM

More information

CP Violation in B Decays at Belle

CP Violation in B Decays at Belle Journal of Physics: Conference Series CP Violation in B Decays at Belle To cite this article: Masaya Iwabuchi J. Phys.: Conf. Ser. 335 37 View the article online for updates and enhancements. Related content

More information

ub + V cd V tb = 0, (1) cb + V td V

ub + V cd V tb = 0, (1) cb + V td V REVIEW OF β, α AND γ MEASUREMENTS K. TRABELSI KEK (High Energy Accelerator Research Organization) Institute of Particle and Nuclear Studies 1-1 Oho, Tsukuba-shi, Ibaraki-ken, 35-81, Japan Precision measurements

More information

RESULTS FROM B-FACTORIES

RESULTS FROM B-FACTORIES XL International Meeting on Fundamental Physics Benasque, May 12 RESULTS FROM B-FACTORIES (IFIC Valencia) τ - τ + τ - τ + B factories KEKB s=10.58 GeV e + e- Υ(4s) Υ(4s) B B z ~ c βγ τ B ~ 200µm BaBar

More information

Measurement of forward-rapidity heavy-flavour muons in proton-proton collisions at s = 7 TeV with ALICE

Measurement of forward-rapidity heavy-flavour muons in proton-proton collisions at s = 7 TeV with ALICE Measuremen of forward-rapidiy heavy-flavour muons in proon-proon collisions a s = 7 TeV wih ALICE D. Socco for he ALICE Collaboraion Ecole des Mines, CNRS-IN2P3, Universié de Nanes Nanes, France Ocober

More information

Hiroyuki Sagawa KEK OHO 1-1, Tsukuba, Ibaraki, Japan

Hiroyuki Sagawa KEK OHO 1-1, Tsukuba, Ibaraki, Japan Hiroyuki Sagawa KEK OHO 1-1, Tsukuba, Ibaraki, Japan In the neutral B meson system, it is possible to measure the CKM angle α using the decay mode b uud in the presence of penguin pollution. Here the recent

More information

Time-dependent CP violation

Time-dependent CP violation Time-dependent CP violation experimental results and prospects Paul Seyfert on behalf of the collaboration INFN Milano Bicocca 13th October 216 Paul Seyfert (INFN MIB) time dependent CPV implications workshop

More information

La Fisica dei Sapori Pesanti

La Fisica dei Sapori Pesanti La Fisica dei Sapori Pesanti Lina Barbaro Galtieri Simposio in onore di Romano Bizzarri Roma, La Sapienza, 10 Febbraio 2004 Lina Galtieri Simposio in onore di Romano Bizzarri, Roma 10 Febbraio 2004 1 Heavy

More information

CP Violation in B Decays at BABAR

CP Violation in B Decays at BABAR CP Violation in B Decays at BABAR October 19-, 11 October 19-, 11 CP Violation in B Decays at BABAR (page 1 B Meson Factories BABAR at SLAC National Accelerator Laboratory, California, USA Another B-factory

More information

Latest time-dependent CP-violation results from BaBar

Latest time-dependent CP-violation results from BaBar Latest time-dependent CP-violation results from BaBar Owen Long, UC Santa Barbara TM All results are preliminary XXXVIIth Rencontres de Moriond QCD and Hadronic Interactions March 17, 2002 The CKM matrix

More information

Cracking the Unitarity Triangle

Cracking the Unitarity Triangle Cracking the Unitarity Triangle Latest Results from BABAR Masahiro Morii Harvard University NEPPSR 2004, Craigville, MA Unitarity Triangle Already seen it a few times this week VV + VV + VV = 0 ud ub cd

More information

BABAR Status & Physics Reach in Coming Years

BABAR Status & Physics Reach in Coming Years BABAR Status & Physics Reach in Coming Years Gautier Hamel de Monchenault CEA-Saclay DAPNIA/SPP on behalf of the BABAR Collaboration CERN, 14 February 2006 Status of PEP-2 and BABAR PEP-2 and BABAR at

More information

CHROMOMAGNETIC AND CHROMOELECTRIC DIPOLE MOMENTS OF THE TOP QUARK IN THE 4GTHDM

CHROMOMAGNETIC AND CHROMOELECTRIC DIPOLE MOMENTS OF THE TOP QUARK IN THE 4GTHDM CHROMOMAGNETIC AND CHROMOELECTRIC DIPOLE MOMENTS OF THE TOP QUARK IN THE 4GTHDM ALAN IGNACIO HERNÁNDEZ JUÁREZ, AGUSTÍN MOYOTL ACUAHUITL AND GILBERTO TAVARES VELASCO FCFM, BUAP XXXII REUNIÓN ANUAL DIVISIÓN

More information

Vub. Longstanding discrepancy between exclusive and inclusive V ub. V ub / V cb constrains the length of the unitarity triangle opposite the angle β.

Vub. Longstanding discrepancy between exclusive and inclusive V ub. V ub / V cb constrains the length of the unitarity triangle opposite the angle β. The V ub puzzle The V ub puzzle Λ b B PDG version 4 6 8 1 1 14 d b u W Vub d u Eclusive π + l νl p b Inclusive W.5.3.35.4.45.5.55 V ub Vub u Xu l νl Longstanding discrepancy between eclusive and inclusive

More information

Advances in Open Charm Physics at CLEO-c

Advances in Open Charm Physics at CLEO-c Advances in Open Charm Physics at CLEO-c Paras Naik CLEO-c 2230104-002 Solenoid Coil Barrel Calorimeter Ring Imaging Cherenkov Detector Drift Chamber Inner Drift Chamber / Beampipe SC Quadrupole Pylon

More information

arxiv: v1 [hep-ex] 10 Oct 2011

arxiv: v1 [hep-ex] 10 Oct 2011 Proceedings of he DPF-11 Conference, Providence, RI, Augus 83, 11 1 Top Quark Resuls Using CMS a 7 TeV K. M. Ecklund Deparmen of Physics and Asronomy, Rice Universiy, Houson, TX, USA I give an overview

More information

BABAR results on Lepton Flavour Violating (LFV) searches for τ lepton + pseudoscalar mesons & Combination of BABAR and BELLE LFV limits

BABAR results on Lepton Flavour Violating (LFV) searches for τ lepton + pseudoscalar mesons & Combination of BABAR and BELLE LFV limits BABAR results on Lepton Flavour Violating (LFV) searches for τ lepton + pseudoscalar mesons & Combination of BABAR and BELLE LFV limits Swagato Banerjee 9 th International Workshop on Tau Lepton Physics

More information

IFAE 2003 Lecce. Alessio Sarti University and INFN Ferrara. BaBar CLEO. Motivation. Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions

IFAE 2003 Lecce. Alessio Sarti University and INFN Ferrara. BaBar CLEO. Motivation. Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions Measuring V ub @ B-factoriesB BaBar Motivation CLEO Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions IFAE 2003 Lecce Belle Alessio Sarti University and INFN Ferrara Motivation Measurements

More information

Measuring α with the B-factories. Adrian Bevan SCIPP 17 th Feb 04

Measuring α with the B-factories. Adrian Bevan SCIPP 17 th Feb 04 Measuring α with the B-factories Adrian Bevan SCIPP 17 th Feb 4 Outline CP Violation in Meson Decay & measuring α Experiments and Techniques measurements in the B meson system: B ππ from Belle and BaBar

More information

Recent Results from BaBar

Recent Results from BaBar Recent Results from BaBar BEACH 2008 Conference Columbia, South Carolina David Norvil Brown University of Louisville Recent Results From BaBar Physics Reach B-physics CP Violation & Mixing, CKM matrix

More information

Review of Standard Tau Decays from B Factories

Review of Standard Tau Decays from B Factories Review of Standard Tau Decays from B Factories Fabrizio Salvatore, RHUL Tau mass measurement Tau decays to strange particles: - Measurement of V us using τ s decays - τ KKπν τ, KKKν τ branching fractions

More information

b s Hadronic Decays at Belle

b s Hadronic Decays at Belle b s Hadronic Decays at Belle Sunghyon Kyeong Yonsei University, Seoul, Korea (on Behalf of the Belle Collaboration Europhysics Conference on High Energy Physics Kraków, Poland, 16- July, 9 sunghyon.kyeong@gmail.com

More information

new measurements of sin(2) & cos(2) at BaBar

new measurements of sin(2) & cos(2) at BaBar new measurements of sin(2) & cos(2) at BaBar, UC Irvine For the BaBar collaboration ICHEP24 August 16th, Beijing bruinsma@slac.stanford.edu Decay rates of B mesons 2 Time-dependent rates for B (f + ) or

More information

IFAE 2003 Lecce. Alessio Sarti University and INFN Ferrara. BaBar CLEO. Motivation. Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions

IFAE 2003 Lecce. Alessio Sarti University and INFN Ferrara. BaBar CLEO. Motivation. Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions Measuring V ub @ B-factoriesB BaBar Motivation CLEO Inclusive V ub Exclusive V ub Summary, Outlook and Conclusions IFAE 2003 Lecce Belle Alessio Sarti University and INFN Ferrara Motivation Measurements

More information

Motivation Fit Method Inputs Results Conclusion

Motivation Fit Method Inputs Results Conclusion Motivation Fit Method Inputs Results Conclusion MOTIVATION In the hunt for New Physics (Supersymmetry) the Standard Model (SM) has to be scrutinized in various areas Two very promising areas are CP violation

More information

SEARCH FOR CP VIOLATION IN

SEARCH FOR CP VIOLATION IN BELLE SEARCH FOR CP VIOLATION IN RADIATIVE AND HADRONIC D DECAYS AT BELLE Tara Nanut on behalf of the Belle Collaboration The XIIIth International Conference on Heavy Quarks and Leptons 6 May 16 1 { Tara

More information

Searches for Leptonic Decays of the B-meson at BaBar

Searches for Leptonic Decays of the B-meson at BaBar Searches for Leptonic Decays of the B-meson at BaBar Stephen Jacob Sekula (MIT) on behalf of the BaBar collaboration Presented at Frontiers in Contemporary Physics III Vanderbilt University May 22-28,

More information

Experimental Status of sin2β Measured from b s Penguin Decays. Mathew Graham SLAC FPCP06: Vancouver April 9, 2006

Experimental Status of sin2β Measured from b s Penguin Decays. Mathew Graham SLAC FPCP06: Vancouver April 9, 2006 Experimental Status of sin2β Measured from b s Penguin Decays Mathew Graham SLAC FPCP06: Vancouver April 9, 2006 Time-Dependent CP-Violation b B 0 A f W+ f CP A CP ( Δt) = Γ B f Γ B f ( ) Γ B f ( ) + Γ

More information

CP Violation in the B(s) meson system at LHCb Julian Wishahi on behalf of the LHCb collaboration

CP Violation in the B(s) meson system at LHCb Julian Wishahi on behalf of the LHCb collaboration CP Violation in the B(s) meson system at Julian Wishahi on behalf of the collaboration 5th Rencontres de Moriond, Electroweak Session, 2th of March 215 CPV in Interference of Mixing/Decay interference

More information

How well do we know the Unitarity Triangle? An experimental review

How well do we know the Unitarity Triangle? An experimental review SLAC-PUB-1281 hep-ex/78.3238 September 27 How well do we know the Unitarity Triangle? An experimental review Massachusetts Institute of Technology, Department of Physics, Room 26-443, 77 Massachusetts

More information

CKM phase and CP Violation in B Decays

CKM phase and CP Violation in B Decays CKM phase and CP Violation in B Decays David Brown Lawrence Berkeley National Lab BaBar Collaboration August 14, 2007 Daegu, Korea Talk Outline Review of CPV in the B system Results on the CKM unitarity

More information

Measurement of CP violation in B J/ψK 0 S. decays. Frank Meier TU Dortmund. XXIX Rencontres de Physique de la Vallée d Aoste March 1 7, 2015

Measurement of CP violation in B J/ψK 0 S. decays. Frank Meier TU Dortmund. XXIX Rencontres de Physique de la Vallée d Aoste March 1 7, 2015 Measurement of CP violation in B J/ψK S decays at LHCb Frank Meier TU Dortmund on behalf of the LHCb Collaboration XXIX Rencontres de Physique de la Vallée d Aoste March 1 7, 215 CP violation in the SM

More information

Results on Tau Physics from BaBar

Results on Tau Physics from BaBar Results on Tau Physics from BaBar Eric Torrence University of Oregon Search for Lepton Flavor Violation Study of τ 3h 2h + ν τ (5 prong) Tau Lifetime The BaBar Experiment Integrated Luminosity (fb -1 )

More information

Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron

Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØ Collaborations Outline

More information

CP violation in charmless hadronic B decays

CP violation in charmless hadronic B decays CP violation in charmless hadronic B decays Wenbin Qian University of Warwick UK Flavour 2017, Durham Charmless b decays No charm quark in final state particles ~ 1% of b decay Large CPV from mixing and

More information

Probing beyond the Standard Model with B Decays

Probing beyond the Standard Model with B Decays Probing beyond the Standard Model with B Decays J. Chauveau LPNHE Univ. Paris 6-7 On behalf of the BABAR Collaboration ICHEP 2004, Aug. 16 th 22 nd, 2004 Beijing, China ICHEP'04 Aug. 16-22 J. Chauveau

More information

B Factories. Alan Watson University of Birmingham, UK

B Factories. Alan Watson University of Birmingham, UK Towards (φ ) and γ (φ ) at the 2 3 B Factories Alan Watson University of Birmingham, UK The Unitarity Triangle Source of CP in the Standard Model 1 λ 2 /2 λ Aλ 3 (ρ iη) V CKM λ 1 λ 2 /2 Aλ 2 Αλ 3 (1 ρ

More information

Standard Model of Particle Physics

Standard Model of Particle Physics Standard Model of Particle Physics Chris Sachrajda School of Physics and Astronomy University of Southampton Southampton SO17 1BJ UK SUSSP61, St Andrews August 8th 23rd 2006 Contents 1. Spontaneous Symmetry

More information

The Cabibbo-Kobayashi-Maskawa (CKM) matrix

The Cabibbo-Kobayashi-Maskawa (CKM) matrix The Cabibbo-Kobayashi-Maskawa (CKM) matrix Charge-raising current J µ W = ( ν e ν µ ν τ )γ µ (1 γ 5 ) V = A u L Ad L e µ τ + (ū c t)γ µ (1 γ 5 )V Mismatch between weak and quark masses, and between A u,d

More information

A Bayesian Approach to Spectral Analysis

A Bayesian Approach to Spectral Analysis Chirped Signals A Bayesian Approach o Specral Analysis Chirped signals are oscillaing signals wih ime variable frequencies, usually wih a linear variaion of frequency wih ime. E.g. f() = A cos(ω + α 2

More information

Lecture 14 Mixing and CP Violation

Lecture 14 Mixing and CP Violation Lecture 4 Mixing and CP Violation Mixing of neutral K mesons CP violation in K decays T violation and CPT conservation Observation of charm mixing d and s mixing CP violation in decays Mixing of Neutral

More information

Belle Hot Topics. Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr.

Belle Hot Topics. Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr. Belle Hot Topics Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr. 9, 2006 Outline Search for the Purely Leptonic Decay Β τν Results

More information

Measurements of Leptonic B Decays from BaBar

Measurements of Leptonic B Decays from BaBar Measurements of Leptonic B Decays from BaBar Gregory Dubois-Felsmann Caltech for the BaBar collaboration ICHEP 2004 Heavy Quark Mesons and Baryons session Overview Motivations for studying leptonic B decays

More information

CP Violation in B Decays and the CKM Matrix. Emmanuel Olaiya Rutherford Appleton Laboratory Chilton,Didcot,Oxon,OX11 0QX,UK

CP Violation in B Decays and the CKM Matrix. Emmanuel Olaiya Rutherford Appleton Laboratory Chilton,Didcot,Oxon,OX11 0QX,UK XXIV Physics in Collision - Boston, June 27-29, 24 CP Violation in B Decays and the CKM Matrix Emmanuel Olaiya Rutherford Appleton Laboratory Chilton,Didcot,Oxon,OX11 QX,UK ABSTRACT Results by the BaBar

More information

Tests of (non-) Factorization

Tests of (non-) Factorization Tests of (non-) Factorization Sören Prell Iowa State University INT / SLAC Workshop b c nonleptonic Session May 11, 2005 Non-Factorizable B Decays Stuy of moes not ominate by factorizable part of amplitue

More information

Measuring α with B ρρ and ρπ

Measuring α with B ρρ and ρπ Measuring with B ρρ and ρπ Andrei Gritsan LBNL May 14, 2005 U. of WA, Seattle Workshop on Flavor Physics and QCD Outline Minimal introduction = arg[v td Vtb/V ud Vub] with b u and mixing penguin pollution

More information

Measurements of the top quark mass and decay width with the D0 detector

Measurements of the top quark mass and decay width with the D0 detector Proceedings of he DPF-2011 Conference, Providence, RI, Augus 8-13, 2011 1 Measuremens of he op quark mass and decay widh wih he D0 deecor Y. Ilchenko Souhern Mehodis Universiy, Dallas, TX 75206, USA The

More information

Recent V ub results from CLEO

Recent V ub results from CLEO Recent V ub results from CLEO Marina Artuso Representing the CLEO Collaboration Beauty 2005, Assisi, June 20-25, 2005 1 Quark Mixing Weak interaction couples weak eigenstates, not mass eigenstates: CKM

More information

Semileptonic B decays at BABAR

Semileptonic B decays at BABAR at (University of Oregon) representing collaboration March 4, 4 1.5 excluded area has

More information

Chapter 2. Models, Censoring, and Likelihood for Failure-Time Data

Chapter 2. Models, Censoring, and Likelihood for Failure-Time Data Chaper 2 Models, Censoring, and Likelihood for Failure-Time Daa William Q. Meeker and Luis A. Escobar Iowa Sae Universiy and Louisiana Sae Universiy Copyrigh 1998-2008 W. Q. Meeker and L. A. Escobar. Based

More information

Impact of Charm Physics on CKM. David Asner Carleton University

Impact of Charm Physics on CKM. David Asner Carleton University Impact of Charm Physics on CKM David Asner Carleton University Outline 1) Review Benefits of Threshold Running 2) Discuss Two Roles of Charm Physics Precision Decay Rates, Spectra Leptonic, Semileptonic,

More information

SEARCH FOR 4 TH GENERATION QUARKS AT CMS

SEARCH FOR 4 TH GENERATION QUARKS AT CMS SEARCH FOR 4 TH GENERATION QUARKS AT CMS Kai-Feng Chen National Taiwan University LHC symposium in PSROC annual meeting January 6 th 0, National Normal University, Taipei 4TH GENERATIONS: WHY? WHY NOT?

More information

New Physics & Future B Physics Programs CP violation Rare Decays

New Physics & Future B Physics Programs CP violation Rare Decays Andrey Golutvin ARGUS & ITEP/Moscow New Physics & Future B Physics Programs CP violation Rare Decays 1 Experimental Facilities LHCb forward spectrometer (running in pp collider mode) Data taking starts

More information

A.Mordá. INFN - Padova. 7 th July on behalf of the Belle2 Collaboration. CP Violation sensitivity at the Belle II Experiment

A.Mordá. INFN - Padova. 7 th July on behalf of the Belle2 Collaboration. CP Violation sensitivity at the Belle II Experiment A. Mordá CP Violation sensitivity at the Belle II Experiment 7 th July 7 / CP Violation sensitivity at the Belle II Experiment A.Mordá on behalf of the Belle Collaboration INFN - Padova 7 th July 7 Introduction

More information

Charmonium Spectroscopy at BESIII

Charmonium Spectroscopy at BESIII Charmonium Spectroscopy at BESIII Hu Liu (on behalf of the BESIII Collaboration) Institute of High Energy Physics, Beijing, China 8 th QWG @GSI 05-10-2011 Slide 1 Outline Brief Introduction of BEPCII &

More information

CP Violation: A New Era

CP Violation: A New Era CP Violation: A New Era Ringberg Phenomenology Workshop on Heavy Flavors 2/5/23 Yossi Nir (Weizmann Institute of Science) Collaborations with: Yuval Grossman, Zoltan Ligeti, Helen Quinn Sandrine Laplace,

More information

Charmed Baryons. Flavor Physics and CP Violation John Yelton University of Florida

Charmed Baryons. Flavor Physics and CP Violation John Yelton University of Florida May 22 1 FPCP U. Penn Charmed Baryons Flavor Physics and CP Violation 22 University of Florida A review of the experimental results on charmed baryons with an accent on recent results. May 22 2 FPCP U.

More information

Recent CP violation measurements. Advanced topics in Particle Physics: LHC physics, 2011 Jeroen van Tilburg 1/38

Recent CP violation measurements. Advanced topics in Particle Physics: LHC physics, 2011 Jeroen van Tilburg 1/38 Recent CP violation measurements Advanced topics in Particle Physics: LHC physics, 2011 Jeroen van Tilburg 1/38 Recap of last week What we have learned last week: Indirect searches (CP violation and rare

More information

Lecture 2: CPV in B system

Lecture 2: CPV in B system 1/39 Lecture 2: CPV in B system CTEQ Summer School Rhodes, Greece - July 2006 Franco Bedeschi, Istituto Nazionale di Fisica Nucleare Pisa, Italy 2/39 Outline Reminder CKM matrix Basic theory CP violation

More information

Multi-Frequency Sheath Dynamics

Multi-Frequency Sheath Dynamics Muli-Frequency Sheah Dynamics Seven Shannon, Alex Paerson, Theodoros Panagopoulos, Daniel Hoffman, John Holland, Dennis Grimard (Universiy of Michigan) Purpose of research RF plasmas wih muliple frequency

More information

On behalf of M. Bona, G. Eigen, R. Itoh and E. Kou

On behalf of M. Bona, G. Eigen, R. Itoh and E. Kou α,φ 2 γ,φ 3 β,φ 1 On behalf of M. Bona, G. Eigen, R. Itoh and E. Kou Chapter Outline Section: Introduction and goals 2p Section: Methodology Subsection: CKMfitter 2p Subsection: UTfit 2p Subsection: Scanning

More information

First Results from CLEO-c

First Results from CLEO-c First Results from CLEO-c Thomas Coan Southern Methodist University CLEO Collaboration CLEO-c Physics Program D + µ + ν µ Decays Absolute Br(D hadrons) e + e - σ (DD) Summary 1 CLEO-c Physics Focus Heavy

More information

VI Charmless B Decays

VI Charmless B Decays Assessing the Impact of the Asymmetric B Factories http://www.slac.stanford.edu/xorg/ckmfitter The whole paper: (Submitted to Eur.Phys.J.C) I The CKM matrix and the UT triangle V Constraints on 2β + γ

More information

Heavy Quark Physics. Cracking the Standard Model? Matthias Neubert Cornell University. CTEQ Summer School 2005 Puebla Mexico May 2005

Heavy Quark Physics. Cracking the Standard Model? Matthias Neubert Cornell University. CTEQ Summer School 2005 Puebla Mexico May 2005 Heavy Quark Physics Cracking the Standard Model? Matthias Neubert Cornell University CTEQ Summer School 2005 Puebla Mexico May 2005 May 25, 2005 CTEQ Summer School 1 Lecture 1 Flavor questions Beyond the

More information

τ Physics at B-factories.

τ Physics at B-factories. τ Physics at B-factories. University of Oregon March, 006 B-factories are τ-factories Standard Model tests Analysis of hadronic τ decays Searches for lepton flavour violating τ decays τ physics at Υ(4S)

More information

ωω: J. Albert Caltech March 24, 2006

ωω: J. Albert Caltech March 24, 2006 ωω: Search for B 0 ωφ and B 0 ωω Are CP and polarization in loops consistent Are CP and polarization in loops consistent with the Standard Model? with the Standard Model? March 24, 2006 J. Albert Caltech

More information

Single Higgs production at LHC as a probe for an anomalous Higgs self coupling

Single Higgs production at LHC as a probe for an anomalous Higgs self coupling Sinle is producion a LC as a probe for an anomalous is self couplin Pier Paolo Giardino Brookhaven Naional Laboraory ICEP 2016, Chicao Based on arxiv:1607.0425 [hep-ph]; Giuseppe Derassi, P.P.G, Fabio

More information

Summary of WG5. Gianluca Cavoto. INFN Roma La Sapienza. On behalf of WG5 conveners Robert Fleischer Karim Trabelsi Jure Zupan

Summary of WG5. Gianluca Cavoto. INFN Roma La Sapienza. On behalf of WG5 conveners Robert Fleischer Karim Trabelsi Jure Zupan Summary of WG5 Gianluca Cavoto INFN Roma La Sapienza On behalf of WG5 conveners Robert Fleischer Karim Trabelsi Jure Zupan CKM Workshop 2006 in Nagoya 1 Overview The charge The main goal is the measurements

More information

B the Tevatron

B the Tevatron B Physics @ the Tevatron Stephanie Hansmann-Menzemer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg DESY, 9 th of November 7 xxx p.1/1 Tevatron p p collisions at s = 1.96 TeV observed by

More information

An Analysis of Supersymmetric Effects on B φk Decays in the PQCD Approach

An Analysis of Supersymmetric Effects on B φk Decays in the PQCD Approach An Analysis of Supersymmetric Effects on B φk Decays in the PQCD Approach Satoshi Mishima (Nagoya Univ.) S. M. and A. I. Sanda, accepted in PRD. [hep-ph/31168] S. M. and A. I. Sanda, Prog. Theor. Phys.

More information