Physics of the Charm Quark Gene Golowich Physics Department Univ. of Massachusetts Amherst MA Colloquium Wayne State Univ. September 22, 2005.

Slides:



Advertisements
Similar presentations
Excited Charm and K0sK0s Resonance Production at ZEUS V. Aushev For the ZEUS Collaboration XXXIX International Symposium on Multiparticle Dynamics ''Gold.
Advertisements

Recent results on quarkonium spectroscopy from BaBar and Belle Bryan Fulsom SLAC National Accelerator Laboratory XXIII iemes Rencontres de Blois Blois,
Properties and Decays of Heavy Flavor S-Wave Hadrons Rohit Dhir Department of Physics, Yonsei University, Seoul Dated:11 th June, 2012.
Heavy quark spectroscopy and accurate prediction of b-baryon masses in collaboration with Marek Karliner, B. Keren-Zur and J. Rosner H.J. Lipkin.
Branching Ratios of B c Meson Decaying to Vector and Axial-Vector Mesons Rohit Dhir Department of Physics, Yonsei University, Seoul, Korea. Dated:21-Sept-2012.
Charm results overview1 Charm...the issues Lifetime Rare decays Mixing Semileptonic sector Hadronic decays (Dalitz plot) Leptonic decays Multi-body channels.
S-Waves & the extraction of  s Sheldon Stone FPCP 2010, Torino, Italy, May 2010.
CHARM-2007, Ithaca, NY Alexey Petrov (WSU) Alexey A. Petrov Wayne State University Table of Contents: Introduction CP-violation in charmed mesons Observables.
ICFP 2005, Taiwan Colin Gay, Yale University B Mixing and Lifetimes from CDF Colin Gay, Yale University for the CDF II Collaboration.
Spectroscopy of Heavy Quarkonia Holger Stöck University of Florida Representing the CLEO Collaboration 6 th International Conference on Hyperons, Charm.
Current Methods of determining V ub I. Endpoint of the inclusive lepton spectrum II. Exclusive decays Methods of determining V ub with small theoretical.
Sep. 29, 2006 Henry Band - U. of Wisconsin 1 Hadronic Charm Decays From B Factories Henry Band University of Wisconsin 11th International Conference on.
Oct.,  Overview of the CLEO experiment  D and D S leptonic decays to  and  : Measurements of absolute branching fractions Measurements of absolute.
1 V cb : experimental and theoretical highlights Marina Artuso Syracuse University.
Recent Charm Results From CLEO Searches for D 0 -D 0 mixing D 0 -> K 0 s  +  - D 0 ->K *+ l - Conclusions Alex Smith University of Minnesota.
New Results and Prospects of Light Hadron Spectroscopy Shan JIN Institute of High Energy Physics (IHEP) Presented by Yi-Fang Wang.
1 B Physics at CDF Junji Naganoma University of Tsukuba “New Developments of Flavor Physics“ Workshop Tennomaru, Aichi, Japan.
FPCP 2002 May Alexey Petrov (Wayne State Univ.) Theory of D 0 - D 0 mixing Alexey A Petrov Wayne State University Table of Contents: Introduction.
B Decays to Open Charm (an experimental overview) Yury Kolomensky LBNL/UC Berkeley Flavor Physics and CP Violation Philadelphia, May 18, 2002.
Jochen Dingfelder, SLAC Semileptonic Decay Studies with B A B AR Annual DOE HEP Program Review, June 5-8, 2006, SLAC B D   X c,X u.
Elisabetta Barberio University of Melbourne Beauty 2006: Oxford September 2006 Measurements of V cb and Form Factors.
Su Houng Lee – (ExHIC coll.) 1. Recent findings of “Multiquark states” + several comments 2. Statistical vs Coalescence model for hadron production 3.
D 0 D 0 bar Mixing and CP Violation at BESIII Kanglin He June 2006, Beijing.
Structure of the exotic heavy mesons Makoto Takizawa (Showa Pharmaceutical Univ.) Collaborators Sachiko Takeuchi (Japan College of Social Work) Kiyotaka.
1 Charm Results from FOCUS Kihyeon Cho Kyungpook National University Daegu, Korea (On behalf of FOCUS Collaborations) Flavor Physics CP Violation 2004.
Introduction to Flavor Physics in and beyond the Standard Model
Theoretical comments on mixing V.Shevchenko (ITEP) 42d Rencontres de Moriond, La Thuile, Italy, March
Test Z’ Model in Annihilation Type Radiative B Decays Ying Li Yonsei University, Korea Yantai University, China Based on J. Hua, C.S Kim, Y. Li, arxiv:
Non-standard mesons in BES III?
Kraków, June 9th, 2015 Exotic quarkonium-like states Andrzej Kupsc Positronium – quarkonia XYZ studies at BESIII Zc states: Zc 0± (3900), Zc 0± (4020)
BaBar physics, recent highlights and future prospects Owen Long, BaBar physics analysis coordinator U. C. Riverside & SLAC December 5, 2008.
C.H. Chang, ITP, AS Beijing1 Chao-Hsi Chang ( 张肇西 Zhao-XiZhang) I.T.P., Chinese Academy of Sciences 1.Introduction (the meson.
Physical Program of Tau-charm Factory V.P.Druzhinin, Budker INP, Novosibirsk.
1 Highlights from Belle Jolanta Brodzicka (NO1, Department of Leptonic Interactions) SAB 2009.
K.K. Gan The Ohio State University New Results on  Lepton July 17, 2003.
Inclusive four charm hadron production at Belle June 16-20, 2005 International Conference on QCD and Hadronic Physics, Beijing JUNGIL LEE.
QFD, Weak Interactions Some Weak Interaction basics
Charm Physics Potential at BESIII Kanglin He Jan. 2004, Beijing
3/13/2005Sergey Burdin Moriond QCD1 Sergey Burdin (Fermilab) XXXXth Moriond QCD 3/13/05 Bs Mixing, Lifetime Difference and Rare Decays at Tevatron.
Decay properties of D and D s mesons Bhavin Patel Department of Physics Sardar Patel University Vallabh Vidyanagar , Gujarat, INDIA.
B Masses and Lifetimes at the Tevatron Satoru Uozumi University of Tsukuba Duke University.
Inclusive semileptonic B decays: experimental Elisabetta Barberio University of Melbourne FPCP: Vancouver April 2006.
1 Heavy Flavor Physics At the Tevatron Cheng-Ju S. Lin (Fermilab ) Aspen Winter Conference Aspen, Colorado 13 February 2006.
Achim Stahl RWTH Aachen University Beijing, June 2006.
Andrzej Bożek (IFJ PAN, Kraków) B hadron decays to open charm production in B-factories BEACH B hadron decays to open charm production in B-factories.
B s Mixing Parameters and the Search for CP Violation at CDF/D0 H. Eugene Fisk Fermilab 14th Lomonosov Conference Moscow State University August ,
Stephen Lars Olsen Seoul National University February 10, 2014 A New Spectroscopy of Hadrons High-1 Gangwando.
Hadron 2015 / A. Valcarce1/19 Unraveling the pattern of XYZ mesons. Phys. Lett. B 736, 325 (2014) Phys. Rev. Lett. 103, (2009); Phys. Rev. D 79,
Introduction to the Heavy Flavor session XLIst Rencontres de Moriond March QCD and Hadronic interactions at high energy Andrey Golutvin ITEP/CERN.
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.
10/29/2007Julia VelkovskaPHY 340a Lecture 4: Last time we talked about deep- inelastic scattering and the evidence of quarks Next time we will talk about.
Project D: Hidden Charm Exotics at BES III Klaus J. Peters, Institut für Kernphysik, Goethe Universität Frankfurt The QuestBESIII Findings Research GroupWorkpackages.
Mini-workshop at Fukui H. Hayashii (NWU)  Physics at Belle(II) 2014/5/23 1.
Mats Selen, HEP Measuring Strong Phases, Charm Mixing, and DCSD at CLEO-c Mats Selen, University of Illinois HEP 2005, July 22, Lisboa, Portugal.
CHARM2012 experimental summary Stephen Lars Olsen Seoul National University Barrel End-cap.
1 Heavy Flavor Spectroscopy at the Tevatron Ilya Kravchenko MI T.
1 outline ● Part I: some issues in experimental b physics ● why study b quarks? ● what does it take? ● Part II: LHCb experiment ● Part III: LHCb first.
Present status of Charm Measurements
Hadron Physics at Belle
Institute of High Energy physics KEK, Hadron physics at J-PARC, Japan
Spectroscopy Today BaBar’s Contributions
Heavy quark spectroscopy and accurate prediction of b-baryon masses
Theory introduction to charm physics
Charm spectroscopy 1 A. Drutskoy University of Cincinnati
Recent results on light hadron spectroscopy at BES
New insights into from U(3) chiral effective theory
Study of New Hadron Spectroscopy at BESIII
Andrei Nomerotski (Oxford/Fermilab) ICHEP 2006, 29 July 2006
Double Heavy Hadrons at LHC Sino-French Workshop Dec , 2006
Pion transition form factor in the light front quark model
Presentation transcript:

Physics of the Charm Quark Gene Golowich Physics Department Univ. of Massachusetts Amherst MA Colloquium Wayne State Univ. September 22, 2005

Rough Outline Some Background Comments Some Standard Model Some New Physics

‘Coals to Newcastle’ Experiment CLEO: Bonvicini, Cinabro, Dubrovin CDF: Harr, Karchin Theory Petrov, Gabbiani, AlFiky

Discovery of Charm Age: c-quark will turn 31 on 11/11 Birth: East Coast (BNL) West Coast (SLAC) SLAC Method: Narrow resonance at E = 3.1 GeV! Thereafter called the `J/  ’

The Standard Model

NuTeV Anomaly?

Three Years of Tests

Spectrum of Quark Masses Predict this Spectrum: Easy/Hard?

Quark Masses and Theory Predict quark masses? No viable models exist What about String Theory? String ground state huge! `Landscape’ description. Many-universes scenario. Elementary constants random! Lucky us! We EXIST!! What about m c = 1.3 GeV? Difficult theoretically. Not heavy enough! Not light enough! Complications of QCD

QED vs QCD QED QCD

Progress in Lattice QCD

Standard Model Physics D Meson Ground State The spectator c-quark: B c Mesons D Decays: Leptonic, Semileptonic, Nonleptonic Spectroscopy: Exotic states?

D Meson Ground State Predict the States: Easy/Hard?

D Meson Ground State q = u  D 0 q = d  D + q = s  D s + Easy! 3 * of SU(3)

Flavored Mesons Each quark has its own ‘flavor’ Quark composites are ‘flavored’ s-quark: K’s = c-quark: D’s = b-quark: B’s = The t-quark decays too quickly!

B c Mesons!

Leptonic Decay of D + Decay Amplitude: Decay Constant f D : Non-perturbative efect. Requires Lattice QCD!

f D : Theory vs Experiment

Semileptonic Decays Decay Amplitude: D 0  K e + e

Form Factor Slopes

Nonleptonic Decays Decay Amplitude: A = a e i 

Dalitz Studies

Phase Information

More Dalitz

Comparative Lifetimes B: B - = b B 0 = d  - /  0 = 0.92

Comparative Lifetimes B: B - = b B 0 = d  - /  0 = 0.92 D: D 0 = c D + = c  - /  0 = 2.55

Comparative Lifetimes B: B - = b B 0 = d  - /  0 = 0.92 D: D 0 = D + =  - /  0 = 2.55 K: K - = K 0 =  - /  0 = 139.

Charm Production e+e- collisions produce charm. There are predictions for this. Not all data are understood!

Heavy Meson Spectroscopy

X(3872) Sighting

Is X(3872) a Molecule? AlFiky, Gabbiani, Petrov (2005) [plus others] Interpret X(3872) as a bound state of hadrons ( ) Analogous to the Deuteron! Similar molecular state predicted long ago. Beware: other interpretations possible.

Y(3940)  2 /d.o.f. = 15.6/8 stat. sig. = 8.1   above D*D threshold  not found in DD or D*D final states

Is Y(3940) a ‘Hybrid’? Hybrid Meson : Color-octet quark-antiquark couples to color-octet gluon to yield color-singlet hadron

D 0  K -  +

Where are CP Violations?

New Physics and Charm Methodology? Rare Decays of D Mesons Flavor Oscillations CP Violations (not discussed here)

Methodology How to find ‘New Physics’? Study systems where SM signals are small. Ideal for charm: A] Rare Decays B] Flavor Oscillations

D 0   +  - in the SM

Data and D 0   +  -

D 0   0 e + e -

Flavor Oscillations Mixing Mixing also in K 0,B d and B s. Each of these is different!

Two Coupled Penduli

The ‘Spring’

New Physics and Mixing

The Normal Modes Normal Modes Effect of CP: CP EigenstatesCP Eigenstates

Mixing of B d Mesons

Mixing of B s Mesons

Mixing of K Mesons

Mixing of D 0 Mesons

Recent Work on D 0 Mixing Theory: Effect of QCD incorporated into analysis of D 0 mixing by Golowich and Petrov. Work continues. Experiment; Especially interesting are attempts to measure  D at the 1% level.

Summary I The c-quark is a remarkably spry 31 year old! A very active social life: Spectroscopy Flavor oscillations Rare decays CP violation searches After studies at CDF, CLEO, Belle and BaBar will come the long awaited LHC.

Summary II Flavor mixing of D mesons will be a hot topic for both experimenters and theorists. Exotic charm states (hybrid and/or molecular) will continue to attract much attention.