Cracking the Unitarity Triangle
|
|
- Alexina Gardner
- 5 years ago
- Views:
Transcription
1 Cracking the Unitarity Triangle Latest Results from BABAR Masahiro Morii Harvard University NEPPSR 2004, Craigville, MA
2 Unitarity Triangle Already seen it a few times this week VV + VV + VV = 0 ud ub cd cb td tb VV ud VV cd ub cb γ α VV td VV cd β tb cb How is this triangle measured experimentally? Using CP violation, of course, right? August 2004 M. Morii, Harvard 2
3 How to Violate CP Complex coupling constant (= weak phase) CKM matrix in the SM has 1 such phase Interference between 2 diagrams with different phases e.g., tree and penguin diagrams for B 0 K + π (Carlo s talk) With 2 diagrams, the size of the CPV is A CP = 2 A A sin φ sin δ 1 2 A CKM information in the weak phase φ A 1 / A 2 ratio, δ usually not calculable + A weak phase difference strong phase difference Observing CPV doesn t necessarily teach us us much about its its origin August 2004 M. Morii, Harvard 3
4 B 0 Mixing to the Rescue B 0 and B 0 mix, i.e., they turn into each other Weak phase = 2 *2 ( VV tb td ) arg = 2β Mass eigenstates are linear combinations B = p B + q B L H 0 0 B = p B q B 0 0 p + q = B H and B L differ in mass ( m), but not in lifetime ( Γ = 0) A little exercise in QM gives us Pure B 0 state after time t Pure B 0 state after time t b t d W + W mt q mt B B () t = e e cos B i sin B 2 p 2 d t b 0 im t Γt 0 0 p mt mt B B () t = e e i sin B + cos B q im t Γt 0 0 August 2004 M. Morii, Harvard 4
5 Mixing and Interference Pure B 0 state, after time t, decays into a CP eigenstate f CP Both B 0 or B 0 can decay into f CP Interference between mixed and unmixed paths Calculate the CP asymmetry Neat problem for undergrad. QM 0 B 0 B mixing 0 fcp H B = Af f CP 0 fcp H B = Af A () t = = C cos( mt) + S sin( mt) 0 0 N( B ( t) fcp ) N( B ( t) fcp ) CP 0 0 f f N( B ( t) fcp) + N( B ( t) fcp) 2 1 λ 2Imλ q A C S λ η p A f f f f = 2 f = 2 f = f 1+ λf 1+ λf f CP eigenvalue decay term mixing term August 2004 M. Morii, Harvard 5
6 Golden Modes Suppose the decay B 0 f CP goes through a single diagram A CP and A CP differ only by the sign of the weak phase Mixing term q/p is known to be almost pure phase Weak phase is 2β Things get nice and simple C 0, S η sin(2 β 2 φ) f f f q A λ = η = η e CP f f f pacp e 2iβ 2iφ A A CP CP = e = = + A () t = η sin(2β + 2 φ)sin( mt) CP For golden decays, the the amplitude S ff of of the the time-dependent CP CP asymmetry measures the the weak phase f 2iφ August 2004 M. Morii, Harvard 6
7 Measuring CP Violation A 0 0 N( B ( t) fcp ) N( B ( t) fcp ) CP 0 0 f f N( B ( t) fcp ) + N( B ( t) fcp ) () t = = C cos( mt) + S sin( mt) Experiment must do 3 things: Produce and detect B f CP events Typical branching fraction: Need a lot of lot of lot of lot of B s Separate B 0 from B 0 = Flavor tagging Use Υ 4S B 0 B 0 and tag one B Measure the decay time Measure the flight length βγct But B s are almost at rest in Υ 4S decays Solution: Asymmetric B Factory August 2004 M. Morii, Harvard 7
8 Three Ingredients 0 0 N( B ( t) fcp ) N( B ( t) fcp ) CP 0 0 f f N( B ( t) fcp ) + N( B ( t) fcp ) A () t = = C cos( mt) + S sin( mt) e Ingredient #1: Signal reconstruction Υ(4S) B reco B 0 e + B 0 µ + e µ - B tag π - Ingredient #2: Flavor tagging π + z ~ βγc t Ingredient #3: t determination August 2004 M. Morii, Harvard 8
9 Asymmetric B Factory Collides e + e at E CM = m(υ 4S ) but with E(e + ) E(e ) PEP-II: 9 GeV e vs. 3.1 GeV e + βγ = 0.56 The boost allows measurement of t Collides lots of them: 2.4A(e + ) 1.6A(e ) PEP-II luminosity /cm 2 /s = 9.2 Hz/nb That s >3x the design σ ( ee + bb) 1nb August 2004 M. Morii, Harvard 9
10 PEP-II Luminosity Run 4 Run 4 BABAR has accumulated 244 fb 1 of data Run 4 (Sep 03-Jul 04) was a phenomenal success August 2004 M. Morii, Harvard 10
11 Detector: BABAR Charged particle momentum with a drift chamber in a 1.5 T field Photon energy with a CsI(Tl) crystal calorimeter Muons detected after penetrating iron yoke Particle ID with a Cerenkov detector (DIRC in BABAR, aerogel in Belle) Precise vertex with a silicon strip detector August 2004 M. Morii, Harvard 11
12 Physics Results Will walk through the 3 angles and 2 sides VV ud VV cd ub cb γ α VV td VV cd β tb cb Almost everything is PRELIMINARY All ICHEP 2004 results from BABAR/Belle are found at BABAR results use data samples between 80 to 227M BB events August 2004 M. Morii, Harvard 12
13 Angle β from b ccs Golden mode of CP violation Tree diagram dominates No weak phase in decay A CP ( t) = η sin(2 β )sin( mt) f B 0 b d c J/ψ c s d K Clean measurement of angle β 0 cc pair can be J/ψ, ψ 2S, χ c1, or η c They are all CP = 1 sd pair can be K S (CP = +1), K L ( 1), or K *0 (mixed) Total 7730 candidates (78% purity) found in 227 M BB events August 2004 M. Morii, Harvard 13
14 Time-Dependent A CP Fit (cc) K S (CP odd) modes J/ψ K L (CP even) mode sin2β = ± (stat) ± (sys) 205 fb -1 August 2004 M. Morii, Harvard 14
15 Unitarity Triangle CKM fit without sin(2β) measurement CKM fit with sin(2β) measurement Precise measurement of sin2β agree with the SM expectation August 2004 M. Morii, Harvard 15
16 Angle β from b sss b sss decay dominated by the penguin diagram b sss b ccs In the SM, A = A = sin 2 New Physics may enter the loop A CP may not agree! φ K S is pure-penguin Small BF: η K S has tree diagrams too Suppressed by small V ub A CP affected by 0.01 to 0.1 Larger BF: CP CP β b d s φ, η s s d u u W η s d K K 0 0 August 2004 M. Morii, Harvard 16
17 B 0 φ K S B 0 φ K S candidates Time-dependent CP asymmetry B 0 tag 114 ± 12 events B 0 tag A CP S φ = 0.29 ± 0.31(stat) K S Combining φ K S and φ K L together, we get S φk fb -1 = 0.50 ± 0.25(stat) (syst), C = 0.00 ± 0.23(stat) ± 0.05(syst) August 2004 M. Morii, Harvard 17 φk
18 B 0 η'k S B 0 φ K S candidates Time-dependent CP asymmetry B 0 tag B 0 tag 205 fb -1 S C η ' K 0 η ' K 0 = 0.27 ± 0.14(stat) ± 0.03(syst) = 0.21± 0.10(stat) ± 0.03(syst) S is 3.0σ from sin2β from ccs A CP August 2004 M. Morii, Harvard 18
19 Status of Angle β BABAR Belle Measurements of CPV in s-penguin channels improving rapidly Average S < sin2β by 2.7σ (BABAR), 2.4σ (Belle) August 2004 M. Morii, Harvard 19
20 Angle α Consider b uud decay Example: B 0 π + π Decay involves V ub Weak phase γ CP asymmetry should measure b Tree W V ub d u u sin(2β + 2 γ) = sin 2α Not so fast There are penguins Penguin u We can measure sin2α only if the penguins are much smaller than the tree It s about 1/3 in B 0 π + π b V tb W g * V td u d Not so good Is there a better way? August 2004 M. Morii, Harvard 20
21 B 0 ρ + ρ B 0 ρ + ρ has much smaller penguin Known from small B(B 0 ρ 0 ρ 0 ) < (90%C.L.) B(B 0 ρ + ρ ) = (30 ±4 ±5) 10 6 ρ is vector meson η CP depends on the polarization Determine the polarization from decay-angle distribution θ 2 + π π 0 ρ B ρ + θ1 0 π 0 π Longitudinal fraction f L = 0.99 ± 0.03 Almost pure CP eigenstate Φ Longitudinal cos θ cos Transverse sin θ sin fb -1 θ θ August 2004 M. Morii, Harvard 21
22 B 0 ρ + ρ B 0 ρ + ρ candidates Time-dependent CP asymmetry B 0 tag 111 fb -1 B 0 tag S C Simultaneously fit for f L and S, C of the long. component = 0.42 ± 0.42( stat) ± 0.14( syst) long long = 0.17 ± 0.27( stat) ± 0.14( syst) A CP August 2004 M. Morii, Harvard 22
23 Status of Angle α A CP in B 0 ρ + ρ combined with BFs for B 0 ρ + ρ, B + ρ + ρ 0, and B 0 ρ 0 ρ 0 96 ± 10(stat) ± 4(syst) α = deg ± 11(penguin) A promising method for measuring α Agrees with the SM with a large error August 2004 M. Morii, Harvard 23
24 Angle γ Hard to find a good channel that measure γ A lot of not-so-good techniques are being studied Example: B D 0 K, D 0 K S π + π 2 decay diagrams Weak phases differ by γ If D 0 decays into a CP eigenstate, interference violates CP Back to the old question How do we know the relative amplitudes? How do we know the strong phase? August 2004 M. Morii, Harvard 24
25 B D 0 K, D 0 K S π + π Suppose we know the amplitude for D 0 K S π + π as a function of m + = m(k S π + ) and m = m(k S π ) Total decay amplitude should be M m m f m m r e f m m B K K i( δ γ) + (, + ) = (, + ) + B ( +, ) for Sππ M m m f m m r e f m m B K K i( δ+ γ) (, + ) = ( +, ) + B (, + ) for Sππ Experiments must Determine f(m,m + ) from fit to the D 0 K S π + π Dalitz plot Fit the decay rates for B + and B and extract r B, δ and γ August 2004 M. Morii, Harvard 25
26 Status of Angle γ Sensitivity is proportional to r B ~ V ub / V cb small No sensitivity for r B < 0.1 with current statistics Bayesian probability with flat prior gives r B < 0.18 (90% C.L.) Combining D 0 K and D 0 K * 194 fb -1 γ = (88 ± 41± 19 ± 10) Not a precision measurement Future: combine multiple methods to constrain r B better August 2004 M. Morii, Harvard 26
27 The Sides In addition to the angles, we measure the lengths of the sides VV ud VV cd ub cb γ α VV td VV cd β tb cb Uncertainties of the left and right sides are dominated by the smallest CKM elements V ub and V td August 2004 M. Morii, Harvard 27
28 Left Side V ub Rate of b ulv decay is proportional to V ub 2 Leptonic part is free from strong final-state interaction Γ( b u ν ) V 1 Γ ub 2 ( b c ν ) V 50 cb Must suppress 50 larger b clv decays Traditional approach: select events with large lepton energy Endpoint above kinematical limit for the b clv decay Only ~6% of b ulv events are accessible 2 b V ub b c b u u ν August 2004 M. Morii, Harvard 28 E l
29 Lepton Endpoint Select electrons in 2.0 < E l < 2.6 GeV Accurate subtraction of background is crucial! Data taken below the Υ 4S resonance for non-bb background Fit the E l spectrum with b ulv, B Dlv, B D * lv, B D ** lv, etc. to extract Data (continuum sub) MC for BB background Data (eff. corrected) MC B( B X eν ) = (1.73± 0.22 ± 0.33 ) 10 u exp theo Turn into 3 V ub exp theo HQET = (3.94 ± 0.25 ± 0.37 ± 0.19 ) fb -1 August 2004 M. Morii, Harvard 29
30 Hadronic Mass and q 2 E l is not the only kinematic variable available There are 3 independent variables Consider m X (hadronic mass) and q 2 (lepton-neutrino mass 2 ) ~70% of b ulv has m X < m D High efficiency + smaller extrapolation Cut on q 2 is less efficient (~20%) but smaller theoretical errors 2 E q ν m X August 2004 M. Morii, Harvard 30
31 Recoil Method Must reconstruct all decay products to measure m X or q 2 E l was much easier B mesons produced in pairs Reconstruct one B in any mode Rest of the event contains exactly one recoil B Find a lepton in the recoil B Remaining part must be X in B Xlv Calculate m X and q 2 For m X < 1.7 GeV and q 2 > 8 (GeV) 2 BB ( Xlν ) = (0.88 ± 0.14 ± 0.13 ± 0.02 ) 10 u stat exp syst (m,a) syst V ub stat exp syst theo syst lepton = (4.92 ± 0.39 ± 0.36 ± 0.46 ) 10 Fully reconstructed B hadrons August 2004 M. Morii, Harvard 31 b v 3 3 X 80 fb -1
32 Status of V ub Different approaches for V ub pursued to tackle theoretical uncertainty Largest error from the shape function Determined by CLEO measurement of photon energy spectrum in b sγ Future improvement from New techniques More data helps Theoretical progress Better measurement of b sγ 80 fb -1 August 2004 M. Morii, Harvard 32
33 Right Side V td B 0 mixing involves virtual top exchange Once B s mixing rate is measured B 0 mixing rate B s mixing rate What can we do besides waiting for Tevatron? Radiative penguin decays b s/d γ Expect Γ( b dγ ) V Γ( b sγ ) V m m d s 2 td 2 ts V B( B ργ) B( B K γ) = V * + td 6 2 V V td ts 2 2 ts 2 b d W + W - Reachable at B Factories d b August 2004 M. Morii, Harvard 33
34 B ρ γ Main background from non-bb events Jet-like geometry Use event shape variables Neural Net B K * γ is 40 larger Particle ID with the Cherenkov detector Combine ρ + γ, ρ 0 γ and ωγ, assuming Γ = Γ = Γ ( B ρ γ) 2 ( B ρ γ) 2 ( B ωγ) B( B ργ) = (0.6± 0.3± 0.1) < (90%C.L.) 191 fb -1 A little smaller than expected by the SM August 2004 M. Morii, Harvard 34
35 Status of V td B(B ργ) limits the length of the right side Bound comparable to that from the mixing Theory errors from ρ vs. K * form factor difference and weak annihilation Observing B ργ with additional statistics will be very interesting Without theory errors 95% C.L. limit including theory errors August 2004 M. Morii, Harvard 35
36 Summary The unitarity triangle is under attack from all directions Huge data sample allow more and more measurements In addition to sin2β, many measurements are reaching interesting precisions CPV in penguin decays, B ρρ, B ulv, B ργ, Will we crack the unitarity triangle? August 2004 M. Morii, Harvard 36
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 informationLatest 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 informationnew 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 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 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 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 informationB 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 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 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 informationLecture III. Measurement of sin 2 in B K 0 S. Measurement of sin 2 in B + -, B + - Measurement of in B DK. Direct CP Violation
Lecture III Measurement of sin 2 in BK S Measurement of sin 2 in BK S Measurement of sin 2 in B + -, B + - Measurement of in BDK Direct CP Violation Model-independent Test for New Physics Prospects Strategy
More informationCP Violation in B-Meson Decays
K. R. chubert, TU Dresden QNP Jülich, 14/6/ CP iolation in B-Meson Decays CP Discovery in K Decays 1964 Explanation in the tandard Model Expectations for B Decays PEP-II and KEK-B, BABAR and Belle 1: sinß
More informationMeasuring 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 informationRecent 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 informationA.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 informationRecent 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 informationRecent CP violation measurements
Recent CP violation measurements 1/38 Recap of last week What we have learned last week: Indirect searches (CP violation and rare decays) are good places to search for effects from new, unknown particles.
More informationRESULTS 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 informationCP 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 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 informationSUSY-related Lepton and Hadron Flavor Results from Belle Yutaro Sato
SUSY-related Lepton and Hadron Flavor Results from Belle Yutaro Sato For the Belle Collaboration (Nagoya Univ., KMI) 27 th Aug. 2015, SUSY2015 @ Lake Tahoe, USA New physics search at Belle 2 New particles
More informationB 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 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 informationLecture 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 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 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 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 informationNew 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 informationFlavour physics in the LHC era
Maria Laach school, september 2012 An introduction to Flavour physics in the LHC era and quest for New Physics (an experimentalist s point of view) Clara Matteuzzi INFN and Universita Milano-Bicocca 1
More informationRecent results on charmless B and B s decays from Belle
ICHEP 2016 Recent results on charmless B and B s decays from Belle Kamal Jyoti Nath IIT Guwahati, India On behalf of Belle Collaboration August 4, 2016 Kamal J Nath ICHEP 2016 August 4, 2016 1 / 14 Outline
More informationRare 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 informationCP 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 informationCP Violation sensitivity at the Belle II Experiment
CP Violation sensitivity at the Belle II Experiment for the Belle II collaboration Max-Planck-Institut für Physik, München 29th Rencontres de Blois May 30th 2017 The Unitarity Triangle All flavor variables
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 informationObservation of Large CP Violation in the Neutral B Meson System
Observation of Large CP Violation in the Neutral B Meson System Presentation for PHY7357 final exam Yefan Tao Phys.Rev.Lett.87:091802,2001 Background: In 1973, Kobayashi and Maskawa(KM) proposed quark
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 informationBABAR 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 informationIntroduction to Dalitz-plot
Introduction to Dalitz-plot Gagan Mohanty Student Seminar @ TIFR January 7, 01 Few Diversions Hierarchical expansion of CKM (1983) + O( 4) magnitudes d s b phases d s b u c t u c t 3 A triangle at the
More informationG. 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 informationRecent BaBar results on CP Violation in B decays
Journal of Physics: Conference Series OPEN ACCESS Recent BaBar results on CP Violation in B decays To cite this article: Arantza Oyanguren 2013 J. Phys.: Conf. Ser. 447 012029 View the article online for
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 informationImpact of the PXD on the Vertex Reconstruction of π 0 particles
Impact of the PXD on the Vertex Reconstruction of π particles Fernando Abudinén 14. May, 216 1 Why CP-V. Sensitivity to B π π? 2 -Conversions and π e + e 3 Improvement of B Vertex Reco. 4 Summary and Outlook
More informationProbing 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 informationResults of same sign dilepton charge asymmetry from Belle and BaBar
Results of same sign dilepton charge asymmetry from Belle and BaBar Yoshiyuki Onuki High Energy Physics Experiment Group Tohoku University cpv from b factories to tevatron and lhcb@tohoku University Outline
More informationMeasurement 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 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 information15 B-B Mixing and CP Violation
15 B-B Mixing and CP Violation Observation of Mixing and CP Violation Just as for K 0 and K 0, there can be mixing between the B 0 and B 0. In fact, this is possible for two distinct systems, the non-strange
More informationHiroyuki 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 informationCKM 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 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 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 informationPicture Erice. 23 Sept 2002 K. R. Schubert (TU Dresden), QHN Erice
Picture Erice 1 K. R. Schubert, TU Dresden Quarks in Hadrons and Nuclei Erice, 23 Sept 22 Title page New Results on CP Violation in B-Meson Decays Old Results on CPV in K and B Decays Explanation in the
More informationResults 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 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 informationKEKB collider and Belle detector
Belle B τν 1 KEKB collider and Belle detector Located(at(KEK(in(Tsukuba. e + e Υ(S) BB Resistive plate chamber + Fe (detection of μ and K L ) CsI(Tl) calorimeter (detection of e ± and γ) e! e! Four layers
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 informationHadronic 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 informationSearches 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 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 informationMeasuring 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 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 informationCP 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 informationStudies of CP Violation at BABAR
SLAC-PUB-878 BABAR-PROC-/32 hep-ex/1336 February, 21 Studies of CP Violation at BABAR Anders Ryd 1 California Institute of Technology, 356-48, Pasadena CA 91125 (for the BABAR Collaboration) Abstract BABAR
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 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 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 informationMikihiko 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 informationAdrian Bevan Department of Physics Liverpool University Liverpool, United Kingdom (from the BABAR Collaboration.)
BABAR-PROC-04/138 SLAC-PUB-10874 Measurements of sin 2α/φ 2 from B ππ, ρπ and ρρ modes. Adrian Bevan Department of Physics Liverpool University Liverpool, United Kingdom (from the BABAR Collaboration.)
More informationMeasuring 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 informationResults 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 informationLHCb 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 informationMeasurements 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 informationDetermination of UT Angles
CP Violation in treeominate processes an Determination of UT Angles Giancarlo Pirea INFN Roma La Sapienza On behalf of BaBar an Belle Collaborations 5th Rencontres u Vietnam Hanoi, August 6-12, 24 1 B-Physics
More informationStudy of e + e annihilation to hadrons at low energies at BABAR
Study of e + e annihilation to hadrons at low energies at BABAR V.Druzhinin Novosibirsk State University, BINP, Novosibirsk on behalf of the BABAR Collaboration International Symposium Advances in Dark
More informationLecture 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 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 informationPrecision measurement of
Precision of Francesca Dordei University of Heidelberg, Physikalisches Institut b 3rd IMPRS-PTFS Seminar, Heidelberg - 24 th April 2012 (Heidelberg University) 24-04-2012 1 / 24 and the LHCb detector CP
More informationMeasurement of time dependent CP violation in B φks. Mahalaxmi Krishnamurthy University of Tennessee. BaBar Collaboration Beauty 2003
Measurement of time dependent CP violation in B φks Mahalaxmi Krishnamurthy University of Tennessee BaBar Collaboration Beauty 2003 CMU, Pittsburgh 1 b-> sss Decays CP violation from interference of decay
More informationThe Mystery of Vus from Tau decays. Swagato Banerjee
The Mystery of Vus from Tau decays Swagato Banerjee Flavor generations in the Standard Model Vij: Mixing between Weak and Mass Eigenstates 2 Unitarity of the CKM matrix 1!! 3! 1! 2! 3! 2 1 V ud = 0.97408
More informationMeasurement of CP Violation in B s J/ΨΦ Decay at CDF
Measurement of CP Violation in B s J/ΨΦ Decay at CDF Gavril Giurgiu Johns Hopkins University University of Virginia Seminar April 4, 2012 Introduction - CP violation means that the laws of nature are not
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 informationFirst Year of BABAR/PEP-II
First Year of BABAR/PEP-II Measuring CP Violation at an Asymmetric B Factory Masahiro Morii Stanford Linear Accelerator Center Outline Physics What We Measure at BABAR/PEP-II, and Why Why CP Violation?
More informationarxiv: v1 [hep-ex] 10 Aug 2011
The Physics Potential of SuperB F. F. Wilson 1 on behalf of the SuperB Collaboration STFC Rutherford Appleton Laboratory, Chilton, Didcot, Oxon, OX11 0QX, UK arxiv:1108.2178v1 [hep-ex] 10 Aug 2011 SuperB
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 informationLatest results on B DK/Dπ decays from Belle
Latest results on B DK/Dπ decays from Belle Resmi P K (On behalf of Belle Collaboration) Indian Institute of Technology Madras Chennai, INDIA CKM 18 eptember 17, 18 Resmi P K, IIT Madras Latest results
More informationStudies of charmonium production in e + e - annihilation and B decays at BaBar
Studies of charmonium production in e + e - annihilation and B decays at BaBar I. Garzia, INFN Sezione di Ferrara On behalf of the BaBar Collaboration XVI International Conference on Hadron Spectroscopy
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 informatione + e - (1) Silicon Vertex Detector
3.1 GeV (4) Electromagnetic Calorimeter (3) Cerenkov- Detector (2) Drift Chamber (5) 1.5 T Solenoid (6) Instrumented Iron Yoke e + e - (1) Silicon Vertex Detector 9.0 GeV e + e - Colliders as B Factories
More informationCP violation in B decays
CP violation in B decays Philip Clark University of Bristol The BaBar Collaboration Outline Brief introduction to CP violation in the B meson system. The PEP-II storage ring and BaBar detector. Performance
More informationResults from the B-factories (Lecture 2)
Results from the B-factories (Lecture 2) Helmholz International Summer School HEAVY QUARK PHYSICS Bogoliubov Laboratory of Theoretical Physics, Dubna, Russia, August 11-21, 28 1 Previous lecture b c interfering
More informationHadronic vs e + e - colliders
Hadronic vs e + e - colliders Hadronic machines: enormous production of b-hadrons (σ bb ~ 50 µb) all b-hadrons can be produced trigger is challenging complicated many-particles events incoherent production
More informationRecent Results on Radiative and Electroweak Penguin B Decays at Belle. Akimasa Ishikawa (Tohoku University)
Recent Results on Radiative and Electroweak Penguin B Decays at Belle Akimasa Ishikawa (Tohoku University) Introduction Loop processes are sensitive to physics Beyond the Standard Model (BSM) since unobserved
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 informationRecent results from rare decays
Recent results from rare decays Jeroen van Tilburg (Physikalisches Institut Heidelberg) Don t worry about the number of slides: Only half of them is new Advanced topics in Particle Physics: LHC physics,
More informationWolfgang Gradl. on behalf of the BABAR collaboration. Tau 2016, Beijing 23 rd September 2016
ISR K u K u π (π ) Wolfgang Gradl on behalf of the collaboration Tau 216, Beijing 23 rd September 216 Motivation γ µ QED is precision physics u l 1 2 (u 2) l testbed for QED experimentally: electron ok
More informationBeyond Standard Model Effects in Flavour Physics: p.1
Beyond Standard Model Effects in Flavour Physics: Alakabha Datta University of Mississippi Feb 13, 2006 Beyond Standard Model Effects in Flavour Physics: p.1 OUTLINE Standard Model (SM) and its Problems.
More informationLepton Violation Studies and Rare Radiative Decays in BaBar. John M. LoSecco, Notre Dame. for the BaBar Collaboration. Miami 06, December 2006
Lepton Violation Studies and Rare Radiative Decays in BaBar John M. LoSecco Notre Dame for the BaBar Collaboration Miami December 2006 Introduction τ LFV Searches at BaBar τ > µ γ τ > e γ τ >lhh τ >l ll
More informationDecadimenti senza charm e misure di α alle B-Factory
Decadimenti senza charm e misure di α alle B-Factory Marcella Bona INFN e Università di Torino Incontri sulla Fisica delle Alte Energie Quark pesanti Lecce, 24 Aprile 2003 IFAE Lecce, Quark Pesanti, 24
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 informationB-Physics Potential of ATLAS, CMS, LHCb and BTeV
B-Physics Potential of ATLAS, CMS, LHCb and BTeV Neville Harnew University of Oxford 8th International Symposium on Heavy Flavour Physics N.Harnew 29th July 1999 1 Outline Introduction The 2nd Generation
More information