Fernando Martínez-Vidal IFIC, Universidad de Valencia-CSIC Concurso-Oposición CSIC 29 de Septiembre de 2004 BaBar & SuperB Fernando Martínez-Vidal IFIC,

Slides:



Advertisements
Similar presentations
Physics with antiprotons: CP violation in D-mesons Klaus Peters Ruhr-Universität Bochum KVI Groningen Jan 7, 2003.
Advertisements

Measurements of the angles of the Unitarity Triangle at B A B AR Measurements of the angles of the Unitarity Triangle at B A B AR PHENO06 Madison,15-18.
Sharpening the Physics case for Charm at SuperB D. Asner, G. Batignani, I. Bigi, F. Martinez-Vidal, N. Neri, A. Oyanguren, A. Palano, G. Simi Charm AWG.
03 Aug NP041 KOPIO Experiment Measurement of K L    Hideki Morii (Kyoto Univ.) for the KOPIO collaborations Contents Physics Motivation.
MSSM Precision tests of the flavours in the SM Model Indep. Analysis in  B=2 MFV, mainly high tan  scenarios Achille Stocchi (LAL-IN2P3/CNRS)
Charm results overview1 Charm...the issues Lifetime Rare decays Mixing Semileptonic sector Hadronic decays (Dalitz plot) Leptonic decays Multi-body channels.
EPS, July  Dalitz plot of D 0   -  +  0 (EPS-208)  Kinematic distributions in  c   e + (EPS-138)  Decay rate of B 0  K * (892) +  -
Title Gabriella Sciolla Massachusetts Institute of Technology Representing the BaBar Collaboration Beauty Assisi, June 20-24, 2005 Searching for.
Search for B s oscillations at D  Constraining the CKM matrix Large uncertainty Precise measurement of V td  properly constrain the CKM matrix yield.
DPF Victor Pavlunin on behalf of the CLEO Collaboration DPF-2006 Results from four CLEO Y (5S) analyses:  Exclusive B s and B Reconstruction at.
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
Jan 28th, 2009Colin Jessop at Notre Dame An experiment to measure CP violation in B mesons Colin Jessop University of Notre Dame.
Introduction to Single-Top Single-Top Cross Section Measurements at ATLAS Patrick Ryan (Michigan State University) The measurement.
1 B Physics at CDF Junji Naganoma University of Tsukuba “New Developments of Flavor Physics“ Workshop Tennomaru, Aichi, Japan.
1 Physics Case of L=10 36 e + e - B Factory Achille Stocchi LAL-Orsay Université Paris-Sud and IN2P3-CNRS.
Charmonium Decays in CLEO Tomasz Skwarnicki Syracuse University I will concentrate on the recent results. Separate talk covering Y(4260).
Description of BTeV detector Jianchun Wang Syracuse University Representing The BTeV Collaboration DPF 2000 Aug , 2000 Columbus, Ohio.
Moriond EW, 3 Mar 2008Tagir Aushev (EPFL, ITEP)1  B → K S  0  0  B → K S K S  B → K S  0  B → D *+ D *-  B → a 1 , a 1 K, b 1 , b 1 K...  
B Production and Decay at DØ Brad Abbott University of Oklahoma BEACH 2004 June 28-July 3.
DPF 2009 Richard Kass 1 Search for b → u transitions in the decays B → D (*) K - using the ADS method at BaBar Outline of Talk *Introduction/ADS method.
Wolfgang Menges, Queen Mary Measuring |V ub | from Semileptonic B Decays Wolfgang Menges Queen Mary, University of London, UK Institute of Physics: Particle.
Super B KEK - Super KEKB -
SuperKEKB to search for new sources of flavor mixing and CP violation - Introduction - Introduction - Motivation for L= Motivation for L=
Philip J. Clark University of Edinburgh Rare B decays The Royal Society of Edinburgh 4th February 2004.
Status and Physics Prospects of the SuperKEKB Project Y. Horii Tohoku Univ. (Japan) 1 5th March 2011, La Thuile 2011.
Measurement of CP violation with the LHCb experiment at CERN
Scientific Highlights : CDF Experiment 1.Introduction 2.CDF Run-II detector 3.Phyiscs highlights B Physics, Top, Higgs, … to be continued by Rob October.
Rare Charm Decays Adrian Bevan IHEP, Beijing, 22 nd October 2011
Higgs Properties Measurement based on HZZ*4l with ATLAS
M. Adinolfi - University of Bristol1/19 Valencia, 15 December 2008 High precision probes for new physics through CP-violating measurements at LHCb M. Adinolfi.
BaBar physics, recent highlights and future prospects Owen Long, BaBar physics analysis coordinator U. C. Riverside & SLAC December 5, 2008.
Physical Program of Tau-charm Factory V.P.Druzhinin, Budker INP, Novosibirsk.
1 ICHEP’04, Beijing, Aug 16-22, 2004 A. Höcker – sin2  in Loop-Dominated Decays with B A B AR The Measurement of sin2β (eff) in Loop-Dominated B Decays.
C. K. MackayEPS 2003 Electroweak Physics and the Top Quark Mass at the LHC Kate Mackay University of Bristol On behalf of the Atlas & CMS Collaborations.
Pavel Krokovny Heidelberg University on behalf of LHCb collaboration Introduction LHCb experiment Physics results  S measurements  prospects Conclusion.
1 Highlights from Belle Jolanta Brodzicka (NO1, Department of Leptonic Interactions) SAB 2009.
1 Rare Bottom and Charm Decays at the Tevatron Dmitri Tsybychev (SUNY at Stony Brook) On behalf of CDF and D0 Collaborations Flavor Physics and CP-Violation.
ATLAS B-Physics Reach M.Smizanska, Lancaster University, UK
3/13/2005Sergey Burdin Moriond QCD1 Sergey Burdin (Fermilab) XXXXth Moriond QCD 3/13/05 Bs Mixing, Lifetime Difference and Rare Decays at Tevatron.
B Masses and Lifetimes at the Tevatron Satoru Uozumi University of Tsukuba Duke University.
Chunhui Chen, University of Pennsylvania 1 Heavy Flavor Production and Cross Sections at the Tevatron Heavy Flavor Production and Cross Sections at the.
Sep/19/2008 Su Dong Stanford Student Orientation: Accelerator based Particle Physics1 Accelerator Based Particle Physics Su Dong Stanford Student Orientation.
Blair Ratcliff, SLACUS R&D Meeting, Sept. 3, 2008 Blair Ratcliff SLAC Detector R&D: Overview and Opportunities Detector Overview (some old news!). Present.
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
SuperB Adrian Bevan Recontres de Moriond XLIV, La Thuile, Italy 7-14 th March 2009.
RECFA September Kenneth Österberg, University of Helsinki Experimental e + e - physics – LEP&LC DELPHI Major finnish LEP contribution analysis.
Direct CP violation in D  hh World measurements of In New Physics: CPV up to ~1%; If CPV ~1% were observed, is it NP or hadronic enhancement of SM? Strategy:
DØ Beauty Physics in Run II Rick Jesik Imperial College BEACH 2002 V International Conference on Hyperons, Charm and Beauty Hadrons Vancouver, BC, June.
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
Light Hadron Spectroscopy at BESIII Haolai TIAN (On behalf of the BESIII Collaboration) Institute of High Energy Physics, Beijing 23rd Rencontre de Blois.
P Spring 2002 L16Richard Kass B mesons and CP violation CP violation has recently ( ) been observed in the decay of mesons containing a b-quark.
Search for a Standard Model Higgs Boson in the Diphoton Final State at the CDF Detector Karen Bland [ ] Department of Physics,
Living Long At the LHC G. WATTS (UW/SEATTLE/MARSEILLE) WG3: EXOTIC HIGGS FERMILAB MAY 21, 2015.
Beauty and charm at the LHC, Jeroen van Tilburg, FOM Veldhoven 2014 Jeroen van Tilburg Beauty and charm at the LHC: searches for TeV scale phenomena in.
The SuperB Project A major new particle physics centre Fergus Wilson, RAL/STFC On behalf of the SuperB Project STORI 2011, October 11 th 2011.
Measurements of   Denis Derkach Laboratoire de l’Accélérateur Linéaire – ORSAY CNRS/IN2P3 FPCP-2010 Turin, 25 th May, 2010.
Update on & SVT readout chip requirements
D0 mixing and charm CP violation
Tagir Aushev For the Belle Collaboration (EPFL, Lausanne ITEP, Moscow)
New Physics Prospects in Mixing and CP Violation at Belle II
Some toughts on the inputs from Physics
Workshop Goals for the Detector Groups
The SuperB Silicon Vertex Tracker
SVT Issues for the TDR What decisions must be taken before the TDR can be written? What is the mechanism for reaching those decisions How can missing information.
Super-KEKB Collaboration
Representing the BaBar Collaboration
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
Yasuhiro Okada (KEK/Sokendai) October 18, 2007
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
SuperKEKB Proto-collaboration
Presentation transcript:

Fernando Martínez-Vidal IFIC, Universidad de Valencia-CSIC Concurso-Oposición CSIC 29 de Septiembre de 2004 BaBar & SuperB Fernando Martínez-Vidal IFIC, Universitat de València-CSIC IN2P3-MICINN meeting January 12, 2008, Madrid

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 2 Final collisions 12:43pm, Monday 7 Apr 2008 Runs 1-4 Runs published as today 475M Y(4S)  BB

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 3 ×10 enhancement of world sample of Y(3S) & Y(2S) decays Enhance knowledge on spectroscopy –Missing SM  b (nS), h b (nS) –Look for surprises Search for exotic physics, like –Light dark matter candidate  –NMSSM light Higgs a 1

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 4 First strong evidence of D0-D0 mixing (May’07) Unexpected discovery of many new states: +  b (Aug’08) [many of these already published]

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 5  b decays mostly via two gluons, exclusive modes not known Search for bump in photon energy spectrum Consistent with M1 transition ( )

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 6 IFIC, University of Valencia-CSIC (5) –1 Faculty, 2 PhD Staff, 2 Grad University of Barcelona (2) –1 Faculty, 1 Grad LAPP-Annecy (7) –1 Faculty, 2 PhD Staff, 4 Grad Ecole Polytechnique (5) –1 Faculty, 2 PhD Staff, 1 Non-PhD Staff, 1 Grad LAL, Orsay (24) –8 Faculty, 1 PhD Staff, 8 Non-PhD Staff, 7 Grad Saclay (6) –4 PhD Staff, 2 Non-PhD Staff Univ. Paris VI & VII (10) –4 Faculty, 1 PhD Staff, 5 Grad 24 PhD (8.8%) 4 PhD (1.2%) OCF 09 count (based on October 2008) Operating Common Fund Basis

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 The “core” Physics Analysis Program (Intense Analysis Period, ) + Y(nS) Physics (SM & Exotics) Precise extraction of D  Ke,  e, KKe, K  e form factors (LQCD) LAL Publications: PRD 76, (2007), PRD 78, (2008), Eur.Phys.J.C52, 975 (2007) D0 mixing and CPV in D  K S  +  -, K S K+K- (Dalitz method, golden) Measurement of CKM angle  with GLW, ADS and Dalitz (golden) techniques BaBar  combination (Dalitz+ADS+GLW) LAL, LAPP, Ecole Polytech., Paris VI&VII Publications: PRL 95, (2005), PRD 78, (2008), PRD77, (2008), PRD78, (2008),… Measurement of B0 and B+ lifetimes, B0 mixing, and observation of CP Violation Paris VI&VII, LAPP, LAL, Ecole P., Saclay Publications: PRL 87, (2001), PRL87, (2001), PRL 88, (2002), PRD 66, (2002),…

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 8 Estudios fenomenológicos y análisis de datos en el experimento BaBar de la Factoría de B’s de SLAC (EEUU): violación de CP, retorno radiativo y Física del quark charm CICYT-IN2P , CICYT-IN2P F. Martinez-Vidal, IFIC, Valencia – A.M. Lutz, LAL Estudio de las desintegraciones semileptónicas de hadrones charm en el experimento BaBar. MCCIN – IN2P (NUC ) A. Oyanguren, IFIC, Valencia – P. Roudeau, LAL Bilateral funding (history) R-ratio measurement in the BaBar experiment CICYT-IN2P3 2004, E. Grauges, UB – M. Davier, LAL Producción de estados excitados en las desintegraciones semileptónicas de los mesones B y estudio de los sucesos con 4 jets CICYT–IN2P3 PP99-1 ( ) J. Salt, IFIC, Valencia – P. Roudeau, LAL Estudio de la probabilidad de desintegración Z  bb y de las oscilaciones de los mesones B0- B0 mediante técnicas de análisis multidimensional CICYT–IN2P3 PP89-1 ( ) A. Ferrer, IFIC, Valencia – Ch. De la Vaissiere, Paris VI&VII BaBar DELPHI …among others

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 9 If there is New Physics at the TeV scale it must have a flavor/CP structure NP must couple to the SM, and the SM violates flavor New heavy quanta can be detected through precision measurement of processes involving loop diagrams Statistics of O(50 ab -1 ) is necessary to reduce the experimental error below the theoretical uncertainty for the most sensitive analyses Physics reach is complementary to LHCb:  many rare decays are not accessible at LHC  sensitivity to off-diagonal term of squark mixing matrix  test of LFV in  decays BaBar  SuperB/SuperBelle luminosity to have measurable effects (anyhow) if NP particles are at EW scale luminosity to have measurable effects (anyhow) if NP particles are at TeV scale

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 10 Crab waist scheme Small crossing area IP The accelerators

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 11 SuperB/SuperBelle BASELINE OPTION New detector elements (BaBar) Quite similar for SuperBelle (but larger backgrounds) –Photon detection for DIRC quartz bars –Forward PID system (TOF or focusing RICH) –Forward calorimeter crystals (LSO) –Minos-style scintillator for IFR –Electronics and trigger –Computing – large amount of data Babar/Belle has been proved excellent detectors for B-physics  Use same approach and reuse many elements Moderate R&D and engineering required –Small beam pipe technology –Thin silicon pixel detector for first layer (~1 cm, <0.5%X 0, ~100  m) –Drift chamber CF mechanical structure, gas and cell size –Photon detection for DIRC quartz bars Better vertexing & better hermiticity important for many measurements

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 12 6 layers at radius from 1.3 cm to 14 cm, 4× more readout channels than in SVD2 (BELLE): Speed! 2 layers of pixel detectors 4 layers of strips Beam-pipe (r=1cm) SuperBelle Vertex Detector SuperBelle has adopted DEPFET as the technology for the pixel detectors

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 13 Spanish contribution DEPFETs Collaboration Goals: Use DEPFET sensors in ILC vertex detector Recently, use DEPFET in SuperBelle as intermediate project

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 14 SuperB Vertex Detector 40 cm 30 cm 20 cm Layer0 Layer Radius cm cm cm cm to 12.7 cm to 14.6 cm Layer Radius cm cm cm cm to 12.7 cm to 14.6 cm The BaBar SVT technology is adequate for r > 3cm: use design similar to SuperB SVT Layer0 is subject to large backround and needs to be extremely thin: > 5MHz/cm2, 1MRad/yr, < 0.5%X0 Striplets option: mature technology, not so robust against background. Moderate R&D needed on module interconnection/mechanics/FE chip (FSSR2) CMOS MAPS option New & challenging technology Can provide the required thickness Existing devices are too slow Extensive R&D ongoing (SLIM5- Collaboration) on 3-well devices 50x50um 2 Hybrid Pixel Option: tends to be too thick. An example: Alice hybrid pixel module ~ 1% X0 Possible material reduction with the latest technology improvements Viable option, although marginal Layer 0 Layers 1-5

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 15 Plans for SuperB/SuperBelle  We are interested to contribute to SuperB and/or SuperBelle  Good projects for vertex detector construction (as intermediate project before ILC), with similar schedules  SuperBelle: Layers 1-2, DEPFETs (~ )  DEPFET Collaboration  SuperB: Layers 1-5, strips, FE chips (~ )  Good experience and infrastructure, lack of man power (yet)  Very interesting luminosity domain (L>50 ab -1 ) to explore between ~  Decisions to be taken during 2009, for project applications in 2010 B  M H + =350 GeV Higgs-mediated NP in MFV at large tan 

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 16 Venue for the June 2009 BABAR collaboration meeting Valencia June 22nd to 25th, 2009

MCCIN-IN2P3 Meeting, Madrid, 12 nd May, 2008 F. Martinez-Vidal. BaBar & SuperB 17 R D : (3.03  0.16  0.10) x x’ 2 : (-0.22  0.30  0.21) x y’: (9.7  4.4  3.1) x Best fit Best fit,  ’ 2 ≥ 0 + No mixing: (0,0) 1 – CL = 3.17 x (1  ) 4.55 x (2  ) 2.70 x (3  ) 6.33 x (4  ) 5.73 x (5  ) Contours at 1  intervals The no-mixing point is at the 3.9  contour Analysis of the proper time distribution of WS events permits extraction of D 0 mixing parameters y’, x’ 2 Evidence confirmed by Belle and CDF