V ub without shape functions (really!)
|
|
- Leo Montgomery
- 5 years ago
- Views:
Transcription
1 V ub without shape functions (really!) Zoltan Ligeti, Lawrence Berkeley Lab SLAC, Dec. 7, 2001 Introduction... V ub is very important to overconstrain CKM It doesn t really matter in this program whether you measure a CP violating quantity or not. The length of a side is as good as an angle. (M. Wise, hep-ph/ ) Semileptonic B X u l ν rate and spectra... Optimal cuts to eliminate b c background Few comments on nonleptonic B X c/s/ rate ( Campagnari) Summary I will not talk about: Exclusive decays ( Postler / Kronfeld) I will not talk about: Lepton endpoint ( Rothstein)
2 Inclusive semileptonic B decay Operator Product Expansion (OPE): expand decay rates in Λ QCD /m b and α s (m b ) model independent results for sufficiently inclusive observables ( ) { b quark dγ = f(λ } 1, λ 2 ) decay m b m α s (...) + αs(. 2..) +... b Interesting quantities computed to order α s, α 2 sβ 0, and 1/m 2 (1/m 3 used to estimate uncertainties) Good news: Total rates known at few (< 5) percent level (duality...) Improvements: better m b from Υ sum rules / moments of B decay spectra / Lattice Upsilon expansion: (Hoang, ZL, Manohar, PRL , PRD ) V ub = ( ( ) 3.04 ± 0.06 (pert) ± 0.08 (mb ) 10 3 B(B Xu l ν) ) 1/2 1.6 ps τ B Central value: 3.24 (Bigi, Shifman, Uraltsev, ARNPS ); 3.08 (Uraltsev, IJMP A ) Zoltan Ligeti p.1
3 Inclusive B X u l ν decay and V ub Bad news: In certain restricted regions of phase space the OPE breaks down Stringent cuts required to eliminate b c background... and the troubles begin! Proposals to measure V ub : Lepton spectrum: E l > (m 2 B m2 D )/2m B Hadronic mass spectrum: m X < m D Dilepton mass spectrum: q 2 > (m B m D ) 2 q 2 (GeV 2 ) b c allowed Ee>(m2 B -m 2 D )/2m B q 2 >(m B -m D ) 2 (GeV 2 q2 ) b c allowed mx < m D q 2 >(m B -m D ) 2 ν 5 O theory 5 O =breaks= down Ee (GeV) m X (GeV 2 ) Zoltan Ligeti p.2
4 B X u l ν spectra Three qualitatively different regions of phase space: 1) m 2 X E XΛ QCD Λ 2 QCD : the OPE converges, first few terms can be trusted 2) m 2 X E XΛ QCD Λ 2 QCD : infinite set of terms equally important, 2) m 2 X E XΛ QCD Λ 2 QCD : the OPE becomes a twist expansion 3) m X Λ QCD : resonance region cannot compute reliably Both E l > (m 2 B m2 D )/2m B and m X < m D are in (2) since m B Λ QCD m 2 D _1 dγ Γ de l 0.4 (GeV -1 ) _1 dγ _1 dγ Γ dq Γ dm X 0.4 (GeV -2 ) (GeV -2 ) b c b c b c E l (GeV) 2.5 b quark decay to O(α s ) incl. Fermi-motion (model) m X (GeV 2) Experiment happy Theory happy q2 (GeV 2 ) Zoltan Ligeti p.3
5 V ub : q 2 spectrum In large q 2 region, first few terms in OPE can be trusted (Bauer, ZL, Luke, PLB ) Reason: q 2 > (m B m D ) 2 cut implies E X < m D [ m 2 X E XΛ QCD ] Leading and subleading logs of x = m b /(m b q 2 ) were summed (αs n+1 ln n x, x αs n ln n x); results consistent within 1σ (Becher, Neubert, hep-ph/ ) Unknown corrections are O(Λ QCD /m b ) 3 Weak annihilation dominates (Voloshin, PLB ) Guesstimate: 2 3% of b u semileptonic rate; delta-function at maximal q 2 and maximal E l WA o q2 (GeV 2 ) ther O(Λ/m b ) 3 Constrain WA by comparing D 0 vs. D cut s SL widths, or V ub from B ± vs. B 0 decay G G relative error as a function of q 2 Zoltan Ligeti p.4
6 V ub : combine q 2 & m X cuts Can get V ub with theoretical error at 5 10% level, from up to 45% of the events (Bauer, ZL, Luke, PRD ) Such precision can be achieved even with cuts away from the b c threshold Cuts on (q 2, m 2 X ) included fraction error of V ub of b ul ν rate δm b = 80/30 MeV 6 GeV 2, m D 46% 8%/5% 8 GeV 2, 1.7 GeV 33% 9%/6% (m B m D ) 2, m D 17% 15%/12% Compared to pure q 2 cut: expansion in Λ QCD /m c m b Λ QCD /(m 2 b q2 cut) reduced uncertainties from perturbation series and nonperturbative corrections uncertainty from the b quark light-cone distribution function only turns on slowly Zoltan Ligeti p.5
7 Uncertainties (1): perturbation series ε ε included fraction: 1.21 G(q 2 cut, m cut ) (a) The O(ɛ) and O(ɛ 2 BLM ) contributions to G(q2 cut, m cut ), normalized to tree level result, for m cut = 1.86 GeV (solid), 1.7 GeV (short dashed), 1.5 GeV (long dashed) (b) Scale variation: the difference between the perturbative corrections to G(qcut, 2 m cut ), normalized to the tree level result, for µ = 4.7 GeV and µ = 1.6 GeV Zoltan Ligeti p.6
8 Uncertainties (2): b quark mass!"$#%& Fractional effect of ±80 MeV (left) and ±30 MeV (right) uncertainty in m 1S b on G(qcut, 2 m cut ) for m cut = 1.86 GeV (solid line), 1.7 GeV (short dashed line), and 1.5 GeV (long dashed line) Zoltan Ligeti p.7
9 Uncertainties (3): higher dimension operators (showed this before:) 3 ' ' Λ! "$#&%('*),+ #.- /10(2 Estimate of the uncertainties due to dimension-six terms in the OPE as a function of q 2 cut from weak annihilation (solid) and other operators (dashed) Effect of a model structure function on G(q 2 cut, m cut ) as a function of q 2 cut for m cut = 1.86 GeV (solid), 1.7 GeV (short dashed) and 1.5 GeV (long dashed) f(k + ) = aa Γ(a) (1 x)a 1 e a(1 x) a and x related to Λ and λ 1 Zoltan Ligeti p.8
10 V ub from inclusive nonleptonic decay? Disclaimer: I had not thought much about this! C. Campagnari, O. Long et al.: Can one predict B(B X c/s/ )? Some issues: Perturbation series contains logs of m W /m b ; probably better to work to fixed order (αs) 2 and get all terms, than to sum any series ( in the literature) Measurement would eliminate b uūd + s s; this is tiny as predicted by the OPE + perturbation theory makes me more and more and more worried! b c cd charmless: B(B ψ(ns)x s ) = few %, X s X d wins λ 2 20 b dg: seems OK assuming no new physics (ask Alex Kagan) b cūd followed by c d: experimental problem... No obvious show-stopper... [doesn t mean that there isn t a non-obvious one] Zoltan Ligeti p.9
11 Summary Situation for V ub may become similar to present V cb at or below 10% level: Inclusive: neutrino reconstruction seems crucial to obtain q 2 and m X Exclusive: possibly only when unquenched lattice gets there Optimized q 2 and m X cuts can eliminate kinematically allowed region of b c background, while keeping the theory error of V ub close to that of B(B X u l ν) Strategy: (i) reconstruct q 2 and m X ; make cut on m X as large as possible Strategy: (ii) for a given m X cut, reduce q 2 cut to minimize overall uncertainty Would reduce SM allowed range of sin 2β very significantly Zoltan Ligeti p.10
12 Two slides on exclusive V cb (B. Grinstein and Z.L., hep-ph/ )
13 B D ( ) l ν shapes and V cb (1) Correlation between ρ 2 and V cb F (1) is very large assume F ( ) (1) known How to best use constraints from comparing shapes of B D and B D? ρ B D l ν Belle. DELPHI.. OPAL CLEO. ρ B Dl ν CLEO 1997 CLEO 1999 BELLE ALEPH V cb F * (1) ALEPH V cb F(1) 10 2 Zoltan Ligeti p.11
14 B D ( ) l ν shapes and V cb (2) Predictions: [QCD SR: χ 2 (1) 0.04, χ 3(1) 0.02, η(1) 0.6, η (1) 0] ρ 2 F ρ 2 F = ɛ 0.01 ɛ 2 BLM η(1) η (1) χ 2 (1) 3.0 χ 3(1) 0.02 λ 1 /GeV ρ 2 A 1 ρ 2 F = ɛ ɛ 2 BLM η(1) 0.14 η (1) Data: 0.75 χ 2 (1) χ 3(1) λ 1 /GeV Fitted slope parameter CLEO BELLE B D l ν, unitarity constrained fit to ρ 2 A ± 0.11 ± ± 0.17 ± 0.19 B D l ν, linear fit to ρ 2 F 0.98 ± 0.09 ± ± 0.09 ± 0.05 B Dl ν, unitarity constrained fit to ρ 2 F 1.30 ± 0.27 ± ± 0.25 ± 0.15 B Dl ν, linear fit to ρ 2 F 0.76 ± 0.16 ± ± 0.14 ± 0.09 Ultimately want to fit: ρ 2 A 1, ρ 2 F, [c2 A 1, c 2 F ], R 1, R 2 V cb Zoltan Ligeti p.12
Inclusive determinations of V ub and V cb - a theoretical perspective
Inclusive determinations of V ub and V cb - a theoretical perspective Michael Luke University of Toronto March 17, 25 CKM 25 - Workshop on the Unitarity Triangle 1 Global fit, summer 4:.7 η.6.5.4.3.2 excluded
More informationV cb : experimental and theoretical highlights. Marina Artuso Syracuse University
V cb : experimental and theoretical highlights Marina Artuso Syracuse University 1 The method b q W - e, µ, ν c or u q τ Ultimate goal: a precise determination of V cb The challenge: precise evaluation
More informationRecent 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 informationSemileptonic B decays at BABAR
at (University of Oregon) representing collaboration March 4, 4 1.5 excluded area has
More informationB Physics Beyond CP Violation
B Physics Beyond CP Violation Semileptonic B Decays Masahiro Morii Harvard University MIT LNS Colloquium, 2004 Outline Introduction: Why semileptonic B decays? CP violation Unitarity Triangle V ub vs.
More informationDetermination of Vxb
Determination of Vxb Thomas Mannel, Siegen University Workshop on Flavour Dynamics Chamonix, France. October 8-15, 2005 Contents Motivation: Why is Vxb of interest? Exclusive Vcb Heavy Quark Symmetries
More informationTheory of B X u l ν decays and V ub
Inclusive semileptonic B decays 1 Theory of B X u l ν decays and V ub Björn O. Lange Center for Theoretical Physics Massachusetts Institute of Technology Inclusive semileptonic B decays 2 Outline 1. Direct
More informationThe inclusive determination of V ub
The inclusive determination of V ub Paolo Gambino Università di Torino and INFN Torino 1 The Unitarity Triangle V =! V * ij jk ik area= measure of CPV V ud V * ub Unitarity determines several triangles
More informationMarta Calvi Università di Milano Bicocca and INFN Sezione di Milano Piazza della Scienza, Milano, Italy
Marta Calvi Università di Milano Bicocca and INFN Sezione di Milano Piazza della Scienza, 3 20126 Milano, Italy This paper reviews recent results on V cb obtained from exclusive and inclusive B decays
More informationV cb. Determination of. and related results from BABAR. Masahiro Morii, Harvard University on behalf of the BABAR Collaboration
Determination of and related results from BABAR V cb Masahiro Morii, Harvard University on behalf of the BABAR Collaboration V cb from inclusive B semileptonic decays Lepton energy moments Hadron mass
More informationIFAE 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 informationMeasurement of the CKM Sides at the B-Factories
Measurement of the CKM Sides at the B-Factories Wolfgang Menges On behalf of the BaBar and Belle Collaborations Queen Mary, University of London, UK CKM matrix and Unitarity Triangle Semileptonic B decays
More informationIFAE 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 informationThe Future of V ub. Antonio Limosani JSPS Fellow (KEK-IPNS JAPAN) BMN BNM Tsukuba (KEK) Sep Antonio Limosani KEK Slide 1
The Future of V ub Antonio Limosani JSPS Fellow (KEK-IPNS JAPAN) 2010 2006 BMN 2006 BNM Tsukuba (KEK) Sep 13-14 2006 Antonio Limosani KEK Slide 1 Motivation Fundamental parameter in SM L SM =...+ gw µ
More informationRecent 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 informationMeasuring V ub From Exclusive Semileptonic Decays
Measuring V ub From Exclusive Semileptonic Decays Lauren Hsu Cornell University The Lake Louise Winter Institute February 00 1 The Cabibbo-Kobayashi-Maskawa Matrix This matrix describes the (SM) weak couplings
More informationB Physics Beyond CP Violation
B Physics Beyond CP Violation Semileptonic B Decays Masahiro Morii Harvard University University of Illinois Urbana-Champaign HETEP Seminar 3 April 2006 Outline n Introduction: Why semileptonic B decays?
More informationCharm Decays. Karl M. Ecklund
Charm ecays Karl M. Ecklund Outline Results from active experiments BaBar, Belle, CLEO-c, (CF, Ø), FOCUS Guiding principle: Charm s role in flavor physics Hadronic Charm ecays and s branching fractions
More informationSemileptonic B Decays at BABAR
Semileptonic B Decays at BABAR Urs Langenegger (SLAC) April 28, 23 Introduction PEP-II and detector b cl ν B D + l ν NEW Hadronic mass moments b ul ν and V ub Endpoint spectrum Hadronic recoil mass NEW
More informationarxiv:hep-ph/ v1 5 May 1995
CERN-TH/95-107 hep-ph/9505238 May 1995 arxiv:hep-ph/9505238v1 5 May 1995 Uncertainties in the Determination of V cb Matthias Neubert Theory Division, CERN, CH-1211 Geneva 23, Switzerland Abstract I discuss
More informationV ub measurements with the BaBar detector
V ub measurements with the BaBar detector Daniele del Re University of California San Diego (on behalf of the BaBar collaboration) Outline: Inclusive b ulν measurements: Endpoint ν reconstruction m X on
More informationProceedings of the VIIIth International Workshop on Heavy Quarks and Leptons HQL06
Proceedings of the VIIIth International Workshop on Heavy Quarks and Leptons HQL06 October 2006 Deutsches Museum, Munich Editors S. Recksiegel, A. Hoang, S. Paul Organized by the Physics Department of
More informationHeavy 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 informationTowards Precision Flavour Physics
: The Status of Semi-Leptonic B Decays Thomas Mannel CERN PH-TH / Universität Siegen CERN-TH Seminar, May 2008 Contents 1 Introduction 2 External Field Method Results to order 1/m 4 b 3 Towards the O(α
More informationSemileptonic B Decays at BABAR
Semileptonic B Decays at BABAR Urs Langenegger (SLAC) April 23 Introduction Motivation PEP-II and detector b cl ν B D + l ν NEW B( B Xl ν) Moments and OPE Hadronic mass Other methods b ul ν and V ub B
More informationCP 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 informationInclusive B decay Spectra by Dressed Gluon Exponentiation. Einan Gardi (Cambridge)
Inclusive B decay Spectra by Dressed Gluon Exponentiation Plan of the talk Einan Gardi (Cambridge) Inclusive Decay Spectra Why do we need to compute decay spectra? Kinematics, the endpoint region and the
More informationSemileptonic Branching Ratios and Moments
Semileptonic Branching Ratios and Moments Giuseppe Della Ricca University and INFN Trieste, Italy 9 th International Conference on B Physics at Hadron Machines October 14-18, 18, 003 Pittsburgh, PA, USA
More informationShahram Rahatlou University of Rome
Cabibbo-Kobayashi-Maskawa Matrix and CP Violation in Standard Model Shahram Rahatlou University of Rome Lecture 1 Lezioni di Fisica delle Particelle Elementari Many thanks to Vivek Sharma (UCSD) And Achille
More informationHadronic Moments in Semileptonic B Decays from CDFII
Hadronic Moments in Semileptonic B Decays from CDFII Alessandro Cerri Hep-ph/0502003 Accepted for publication in PRDRC Analysis Strategy Typical mass spectrum M(X 0 c ) (Monte Carlo): D 0 and D* 0 well-known
More informationElectroweak Theory: 2
Electroweak Theory: 2 Introduction QED The Fermi theory The standard model Precision tests CP violation; K and B systems Higgs physics Prospectus STIAS (January, 2011) Paul Langacker (IAS) 31 References
More informationPrecision determinations of V cb and V ub
Precision determinations of V cb and V ub Probing weak interactions and CP violation in the quark sector with semileptonic B decays Bob Kowalewski University of Victoria April, 2004 R.V. Kowalewski 1 Outline
More informationMeasurements of V cb, V ub and φ 3 /γ
XXVI Physics in Collision, Búzios, Rio de Janeiro, Brazil, 6-9 July 006 1 Measurements of V cb, V ub and φ 3 /γ M. RóŜańska Institute of Nuclear Physics PAN, Kraków, ul. Radzikowskiego 15, Poland An overview
More informationElectroweak Theory: 5
Electroweak Theory: 5 Introduction QED The Fermi theory The standard model Precision tests CP violation; K and B systems Higgs physics Prospectus STIAS (January, 2011) Paul Langacker (IAS) 162 References
More informationCKM Matrix and CP Violation in Standard Model
CKM Matrix and CP Violation in Standard Model CP&Viola,on&in&Standard&Model&& Lecture&15& Shahram&Rahatlou& Fisica&delle&Par,celle&Elementari,&Anno&Accademico&2014815& http://www.roma1.infn.it/people/rahatlou/particelle/
More informationWeak 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 informationRadiative B meson Decays at BaBar. Colin Jessop University of Notre Dame
Radiative B meson Decays at BaBar Colin Jessop University of Notre Dame Motivations Window to new Physics Help measure the unitarity triangle Test QCD technology Radiative Penguin Decays The Penguin Zoo
More informationCKM ELEMENTS FROM semileptonic b decays
CKM ELEMENTS FROM semileptonic b decays paolo gambino università di torino & INFN Munich 18-21 May 2016 Importance of Vxb Vcb plays an important role in the determination of UT!! " K x V cb 4 +... and
More informationCP 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 informationPart I: Heavy Quark Effective Theory
Part I: Thomas Mannel CERN-PH-TH and Theoretische Physik I, Siegen University KITPC, June 24th, 2008 Contents Motivation 1 Motivation Weak Interaction Reminder Peculiarties of the Standard Model 2 EFT
More informationRadiative and Electroweak Penguin Decays of B Mesons
Radiative and Electroweak Penguin Decays of B Mesons Jeffrey D. Richman University of California, Santa Barbara BABAR AR Collaboration 11 th International Conference on B Physics at Hadron Machines Oxford,
More informationNon-local 1/m b corrections to B X s γ
Non-local 1/m b corrections to B X s γ Michael Benzke TU München September 16, 2010 In collaboration with S. J. Lee, M. Neubert, G. Paz Michael Benzke (JGU) Non-local 1/m b corrections to B X s γ TU München
More informationQCD factorization in B decays ten years later
QCD factorization in B decays ten years later M. Beneke (RWTH Aachen) Flavianet meeting in honour of Chris Sachrajda on the occasion of his 60th birthday Southampton, England, December 14/15, 2009 Early
More informationDetermination of Unitarity Triangle parameters
Determination of Unitarity Triangle parameters Achille Stocchi LAL-Orsay Phenomenology Workshop on Heavy Flavours Ringberg Schloss 8 April May 003 -Introuction (Unitarity Triangle) -The measurements/theoretical
More informationBelle 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 informationVub. 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 informationThe 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 informationAdvances 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 informationarxiv:hep-ph/ Jul 1992
arxiv:hep-ph/9207270 29 Jul 1992 To be published in the Proceedings of the Workshop on B Factories: The State of the Art in Accelerators, Detectors, and Physics, Stanford, California, April 6 10, 1992.
More informationInclusive V ub Measurements at BABAR
SLAC-PUB-115 August 3 hep-ph/37158 Inclusive V ub Measurements at BABAR A. Sarti Representing the BABAR Collaboration Invited talk presented at the nd Workshop on the CKM Unitarity Triangle, 4/5/3 4/9/3,
More informationLeptonic and Semileptonic Charm Decays
Leptonic and Semileptonic Charm Decays Hanna Mahlke Cornell University Heavy Quarks and Leptons Munich, Germany October 006 The Big Picture Theory s difficulties in calculating strong phenomena seriously
More informationParticle Physics. Lecture 12: Hadron Decays.!Resonances!Heavy Meson and Baryons!Decays and Quantum numbers!ckm matrix
Particle Physics Lecture 12: Hadron Decays!Resonances!Heavy Meson and Baryons!Decays and Quantum numbers!ckm matrix 1 From Friday: Mesons and Baryons Summary Quarks are confined to colourless bound states,
More informationB Kl + l at Low Hadronic Recoil
B Kl + l at Low Hadronic Recoil Gudrun Hiller Danny van Dyk Christian Wacker TU Dortmund - Theoretische Physik III DPG-Frühjahrstagung Karlsruhe 11 31. March 11 Christian Wacker (TU Dortmund) B Kl + l
More informationCP Violation Beyond the Standard Model
CP Violation Beyond the Standard Model 5th Recontres du Vietnam Hanoi August 7, 2004 Yossi Nir (Weizmann Institute of Science) Thanks to: Sandrine Laplace, Zoltan Ligeti CPV BSM 1/21 Motivation Why do
More informationStandard 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 informationImpact 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 informationD semi-leptonic and leptonic decays at BESIII
Institute of High Energy Physics, Chinese Academy of Sciences E-mail: mahl@ihep.ac.cn During 2010 and 2011, a data sample of 2.92 fb 1 was accumulated at s = 3.773 GeV by the BESIII detector operating
More informationInclusive B decay Spectra by Dressed Gluon Exponentiation
Inclusive B decay Spectra by Dressed Gluon Exponentiation Plan of the tal Einan Gardi (Cambridge) Inclusive B decay spectra motivation Strategy of the theoretical study Very short introduction to Sudaov
More informationBs studies at a SuperB: physics case and experimental potentialities
Bs studies at a SuperB: physics case and experimental potentialities 1 2 3 4 5 6 E.Baracchini1,2, M.Bona3, F.Ferroni1,2, G.Isidori2,4, G.Martinelli1,2, M.Pierini5, G.Piredda1,2, F.Renga1,2, A.Stocchi6
More informationUnitary Triangle Analysis: Past, Present, Future
Unitarity Triangle Analysis: Past, Present, Future INTRODUCTION: quark masses, weak couplings and CP in the Standard Model Unitary Triangle Analysis: PAST PRESENT FUTURE Dipartimento di Fisica di Roma
More informationCracking 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 informationOn 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 informationProbing Beyond the Standard Model with Flavor Physics
Probing Beyond the Standard Model with Flavor Physics Matthias Neubert Laboratory for Elementary-Particle Physics Cornell University & Institute for Physics Johannes Gutenberg University October 23-31,
More informationQuarkonium Results from Fermilab and NRQCD
Quarkonium Results from Fermilab and NRQCD Paul Mackenzie mackenzie@fnal.gov International Workshop on Heavy Quarkonium Fermilab Sept. 20-22 2003 Thanks Christine Davies (HPQCD), Jim Simone Recent progress
More informationLa 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 informationRare 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 informationCLEO c. Anders Ryd Cornell University June 7, e e cc D D. D K,D K e
CLEOc Cornell University June 7, 25 e e cc D D D K,D K e K K e 1 Outline CLEOc experiment and the physics program Some early results D> Absolute hadronic branching fractions Semileptonic decays 2 Testing
More informationHadronic B decays from SCET
Hadronic B decays from SCET Flavor Physics and CP Violation Conference, Vancouver, 26 1 Christian W. Bauer Ernest Orlando Lawrence Berkeley National Laboratory and University of California, Berkeley, CA
More informationRecent 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 informationApplications of QCD Sum Rules to Heavy Quark Physics
Applications of QCD Sum Rules to Heavy Quark Physics Alexander Khodjamirian UNIVERSITÄT SIEGEN Theoretische Physik 1 RESEARCH UNIT q et f 3 lectures at Helmholtz International School "Physics of Heavy
More informationMoriond QCD La Thuile, March 14 21, Flavour physics in the LHC era. An introduction. Clara Matteuzzi. INFN and Universita Milano-Bicocca
Moriond QCD La Thuile, March 14 21, 2009 Flavour physics in the LHC era An introduction Clara Matteuzzi INFN and Universita Milano-Bicocca 1 Contents 1. The flavor structure of the Standard Model 2. Tests
More informationHow 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 informationLatest Charm Semileptonic Decay Results from CLEO-c
Latest Charm Semileptonic ecay Results from CLEO-c OUTLINE CLEO-c in the context of testing the Standard Model with precision quark flavor physics. ecay constants Form Factors CKM matrix elements K - ν
More informationarxiv:hep-ph/ v4 18 Nov 1999
February 8, 018 arxiv:hep-ph/990998v4 18 Nov 1999 OITS-678 CLEO measurement of B π + π and determination of weak phase α 1 K. Agashe and N.G. Deshpande 3 Institute of Theoretical Science University of
More informationCoupled-channel approach to spin partners of hadronic molecules
Coupled-channel approach to spin partners of hadronic molecules A.V. Nefediev (MIPT, Moscow, Russia) in collaboration with V. Baru, E. Epelbaum, A. A. Filin, F.-K. Guo, C. Hanhart, Yu. S. Kalashnikova,
More informationB D ( ) form factors from QCD sum rules
B D ( ) form factors from QCD sum rules (Master Thesis, June 2008) Christoph Klein in collaboration with Sven Faller Alexander Khodjamirian Thomas Mannel Nils Offen Theoretische Physik 1 Universität Siegen
More informationWhy the is Boring and Why that is Exciting
Why the is Boring and Why that is Exciting Tau Review WIN0 Jean Etienne Duboscq Cornell University Thanks to: T. Browder, M. Davier, S. Eidelman, H. Evans, KK Gan, R. Kass, A. Pich, M. Roney, R. Sobie,
More informationLecture 12 Weak Decays of Hadrons
Lecture 12 Weak Decays of Hadrons π + and K + decays Semileptonic decays Hyperon decays Heavy quark decays Rare decays The Cabibbo-Kobayashi-Maskawa Matrix 1 Charged Pion Decay π + decay by annihilation
More informationDanny van Dyk. B Workshop Neckarzimmern February 19th, Danny van Dyk (TU Dortmund) News on B K µ + µ 1 / 35
News on B K µ + µ Danny van Dyk B Workshop Neckarzimmern February 19th, 2010 Danny van Dyk (TU Dortmund) News on B K µ + µ 1 / 35 The Goal 15 1 10 0.8 5 0.6 C10 0-5 0.4-10 0.2-15 -15-10 -5 0 5 10 15 C
More informationSearch for Physics Beyond the Standard Model at B Factories
Search for Physics Beyond the Standard Model at B Factories Gautier Hamel de Monchenault CEA-Saclay DAPNIA/SPP on behalf of the BABAR & BELLE Collaborations Moskow, 29 July 2006 New Physics in Flavor Sector
More informationBelle II perspectives on Unitarity Triangle sides and angles
Belle II perspectives on Unitarity Triangle sides and angles A.Passeri (INFN Roma Tre) on behalf of the Belle II collaboration EU grant 644294 XIII Meeting on B Physics Marseille october 1 st 2018 01/10/2018
More informationThe CKM matrix elements and their determination. Phil Strother LBL
The CKM matrix elements and their determination Phil Strother LBL Outline Quark mixing, C, and KM V ud V cd V us V cs V cb V ub V tb Some known products of elements Parametrisations, and that phase...
More informationHadron-hadron Interactions
116 PN12 Nov, 2004 Hadron-hadron Interactions general considerations effective approaches microscopic approaches OPE methods Dyson-Schwinger constituent quark model chiral symmetry issues Eric Swanson
More informationConference Summary. K.K. Gan The Ohio State University. K.K. Gan Tau2000 1
Conference Summary K.K. Gan The Ohio State University K.K. Gan Tau2000 1 many interesting results can only summarize some highlights include a few interesting results not presented here apologize to those
More informationPoS(Kruger 2010)048. B X s/d γ and B X s/d l + l. Martino Margoni SLAC-PUB Universita di Padova and INFN
SLAC-PUB-15491 B X s/d γ and B X s/d l + l Universita di Padova and INFN E-mail: martino.margoni@pd.infn.it Flavour Changing Neutral Current transitions B X s/d γ and B X s/d l + l provide an excellent
More informationarxiv: v1 [hep-ph] 23 Oct 2010
QCD challenges in radiative B decays M. Misiak arxiv:1010.4896v1 [hep-ph] 23 Oct 2010 Institute of Theoretical Physics, University of Warsaw, PL-00-681 Warsaw, Poland. Institut für Theoretische Teilchenphysik,
More informationSuperb prospects: Physics at Belle II/SuperKEKB
PANIC July 28, 2011 Superb prospects: Physics at Belle II/SuperKEKB cf G. Varner, talk 3H-1 SuperKEKB & Belle II projects 2 Primary goal: establish unitarity & complex phase of CKM matrix Kobayashi & Maskawa
More informationLong distance weak annihilation contribution to
Long distance weak annihilation contribution to B ± (π/k) ± l + l Sergio Tostado In collaboration with: A. Guevara, G. López-Castro and P. Roig. Published in Phys. Rev. D 92, 054035 (2015). Physics Department,
More informationNew Physics search in penguin B-decays
New Physics search in penguin B-decays Sanjay Swain, SLAC on behalf of BABAR Collaboration 13 th -18 th Dec 2007 Miami 2007 Outline What is New Physics (NP)? b > (d, s) penguin decays Exclusive Semi-inclusive
More informationShort- and mid-distance physics (or quark-hadron duality) from lattice QCD. Shoji Hashimoto (KEK) December 20, Peking University
Short- and mid-distance physics (or quark-hadron duality) from lattice QCD Shoji Hashimoto (KEK) December 20, 2018 @ Peking University QCD is (non-)perturbative perturbative non-perturbative e + e qq Well
More informationQCD, Factorization, and the Soft-Collinear Effective Theory
QCD Factorization and the Soft-Collinear Effective Theory Iain W. Stewart MIT The 9th International Conference on B Physics at Hadron Machines Oct. 14-18 (Beauty 2003) Iain Stewart p.1 Outline Motiviation
More informationSearching for New Physics in Heavy Flavours
Searching for New Physics in Heavy Flavours Luca Silvestrini INFN, Rome Introduction Status of flavour physics in the SM UT beyond the SM and constraints on NP CP violation in Charm Physics Conclusions
More informationAnalysis of the Isgur-Wise function of the Λ b Λ c transition with light-cone QCD sum rules
Analysis of the Isgur-Wise function of the Λ b Λ c transition with light-cone QCD sum rules Zhi-Gang Wang 1 Department of Physics, North China Electric Power University, Baoding 713, P. R. China arxiv:96.426v1
More informationThe 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 informationTheory of hadronic B decays
Theory of hadronic B decays Dan Pirjol MIT BEAUTY 2005, 10th International Conference on B physics Assisi, Italy - 20-24 June 2005 Outline Hadronic B decays - probes of the flavor structure of the Standard
More informationCLEO-c: Recent Results
CLEO-c: Recent Results an Cronin-Hennessy University of Minnesota March 12, 2006 Moriond EW. Cronin-Hennessy, U of M Outline Program Overview CLEOIII Result CLEO-c Leptonic Semileptonic Hadronic. Cronin-Hennessy,
More informationLa Belle Epoque. K.Trabelsi kek.jp Lausanne, 22 Jan, 2009
La Belle Epoque K.Trabelsi karim.trabelsi @ kek.jp Lausanne, Jan, 9 Belle Epoque : was a period in European social history that began during th the late 19 and lasted until World War I... considered as
More informationDiscussion on (Heavy) Flavor Physics
Discussion on (Heavy) Flavor Physics J. Brod, A. Buras, A. El-Khadra, P. Gambino, C. Monahan, A. Petrov Symposium on Effective Field Theories and Lattice Gauge Theory TUM IAS, May 19, 2016 Joachim Brod
More informationReview of semileptonic b clν decays
Review of semileptonic b clν decays Elisabetta Barberio University of Melbourne Seattle 2005 semileptonic spectra b rate shape V cb shape m b,m c µ 2 G, µ 2 π difficulty: go from the measured shape to
More informationReview of Exclusive B D (, ) lν Decays Branching Fractions, Form-factors and V cb
SLAC-PUB-131 hep-ph/7335 April 7 Review of Exclusive B D (, ) lν Decays Branching Fractions, Form-factors and V cb A. E. Snyder Stanford Linear Accelerator Center (SLAC) Menlo Park, CA, USA 91 1 Introduction
More information