Partial Wave Analysis results from JETSET the Jetset experiment

Slides:



Advertisements
Similar presentations
ZEUS high Q 2 e + p NC measurements and high-x cross sections A.Caldwell Max Planck Institute for Physics On behalf of the ZEUS Collaboration Allen Caldwell.
Advertisements

Phi-Psi, Feb.-Mar., 2006, S.Uehara1 Experimental studies of charmonia in two-photon collisions at Belle S.Uehara (KEK) for the Belle Collaboration e +
1 Charged Z’s at Ruslan Chistov (ITEP, Moscow) Representing the Belle Collaboration Quarkonium Working Group Workshop (Nara, NWU, December 2-5/2008) ●
N*(2007) observed at LNS Sendai H. Shimizu Laboratory of Nuclear Science Tohoku University Sendai NSTAR2007, Sep.5-8, 2007, Bonn 1670.
Slepton Discovery in Cascade Decays Jonathan Eckel, Jessie Otradovec, Michael Ramsey-Musolf, WS, Shufang Su WCLHC Meeting UCSB April
G. Cowan RHUL Physics Profile likelihood for systematic uncertainties page 1 Use of profile likelihood to determine systematic uncertainties ATLAS Top.
R Measurement at charm resonant region Haiming HU BES Collaboration Charm 2007 Cornell University Ithaca, NY. US.
Peter Fauland (for the LHCb collaboration) The sensitivity for the B S - mixing phase  S at LHCb.
Study of e + e  collisions with a hard initial state photon at BaBar Michel Davier (LAL-Orsay) for the BaBar collaboration TM.
Measurement of the Branching fraction B( B  D* l ) C. Borean, G. Della Ricca G. De Nardo, D. Monorchio M. Rotondo Riunione Gruppo I – Napoli 19 Dicembre.
Resonances in decay for 400fb -1 DC Meeting April 10th, 2006 J.Brodzicka, H.Palka INP Kraków J.Brodzicka, H.Palka INP Kraków B +  D 0 D 0 K + B +  D.
W  eν The W->eν analysis is a phi uniformity calibration, and only yields relative calibration constants. This means that all of the α’s in a given eta.
1 Introduction to Dijet Resonance Search Exercise John Paul Chou, Eva Halkiadakis, Robert Harris, Kalanand Mishra and Jason St. John CMS Data Analysis.
Analysis of E852 Data at Indiana University Ryan Mitchell PWA Workshop Pittsburgh, PA February 2006.
Irakli Chakaberia Final Examination April 28, 2014.
Chapter 1: Introduction to Statistics
Outline 3  PWA overview Computational challenges in Partial Wave Analysis Comparison of new and old PWA software design - performance issues Maciej Swat.
W+jets and Z+jets studies at CMS Christopher S. Rogan, California Institute of Technology - HCP Evian-les-Bains Analysis Strategy Analysis Overview:
A statistical test for point source searches - Aart Heijboer - AWG - Cern june 2002 A statistical test for point source searches Aart Heijboer contents:
Zijin Guo Univ. of Hawaii Representing BES Collaboration J/    pp and  BES Beijing, China.
1 Tomoaki Hotta (RCNP, Osaka Univ.) for The LEPS Collaboration Cracow Epiphany Conference, Jan 6, 2005 Introduction LEPS experiment Results from new LD.
1 Iterative dynamically stabilized (IDS) method of data unfolding (*) (*arXiv: ) Bogdan MALAESCU CERN PHYSTAT 2011 Workshop on unfolding.
Singa and kappa analyses at BESII Ning Wu Institute of High Energy Physics, CAS Beijing, China January 25-26, 2007.
Trilinear Gauge Couplings at TESLA Photon Collider Ivanka Božović - Jelisavčić & Klaus Mönig DESY/Zeuthen.
The inсlusive produсtion of the meson resonanсes ρ 0 (770), K * (892), f 0 (980), f 2 (1270) in neutrino- nuсleon сharged сurrent (CC) interaсtions Polyarush.
Scalar and pseudoscalar mesons at BESII Xiaoyan SHEN (Representing BES Collaboration) Institute of High Energy Physics, CAS, China Charm06, June 5-7, 2006,
Partial Wave Analysis What is it Relation to physical properties Properties of the S-matrix Limitation and perspectives Examples : peripheral production.
Study of pair-produced doubly charged Higgs bosons with a four muon final state at the CMS detector (CMS NOTE 2006/081, Authors : T.Rommerskirchen and.
1 Searching for Z’ and model discrimination in ATLAS ● Motivations ● Current limits and discovery potential ● Discriminating variables in channel Z’ 
1 Warsaw Group May 2015 Search for CPV in three-bodies charm baryon decays Outline Selections Mass distributions and reconstructed numbers of candidates.
Exclusive ΦΦ in E690 G. Gutierrez FNAL-E690 Collaboration Small-X and Diffraction Physics Conference FERMILAB, Sep 2003.
JPS 2003 in Sendai Measurement of spectral function in the decay 1. Motivation ~ Muon Anomalous Magnetic Moment ~ 2. Event selection 3. mass.
NSTAR2011, Jefferson Lab, USA May 17-20, 2011 Mitglied der Helmholtz-Gemeinschaft Tamer Tolba for the WASA-at-COSY collaboration Institut für Kernphysik.
Mitchell Naisbit University of Manchester A study of the decay using the BaBar detector Mitchell Naisbit – Elba.
Study of e+e- annihilation at low energies Vladimir Druzhinin Budker Institute of Nuclear Physics (Novosibirsk, Russia) SND - BaBar Lepton-Photon, August,
The importance of inelastic channels in eliminating continuum ambiguities in pion-nucleon partial wave analyses The importance of inelastic channels in.
Jin Huang M.I.T. For Transversity Collaboration Meeting Jan 29, JLab.
October 2011 David Toback, Texas A&M University Research Topics Seminar1 David Toback Texas A&M University For the CDF Collaboration CIPANP, June 2012.
Jeroen van Hunen (for the LHCb collaboration) The sensitivity to  s and  Γ s at LHCb.
Nita Sinha The Institute of Mathematical Sciences Chennai.
E. Robutti Enrico Robutti I.N.F.N. Genova HEP 2003 Europhysics Conference July 17-23, Aachen, Germany Recent BABAR results in Charmonium and Charm Spectroscopy.
1 Recent Results on J/  Decays Shuangshi FANG Representing BES Collaboration Institute of High Energy Physics, CAS International Conference on QCD and.
Charm Mixing and D Dalitz analysis at BESIII SUN Shengsen Institute of High Energy Physics, Beijing (for BESIII Collaboration) 37 th International Conference.
A Genetic Algorithm Analysis of N* Resonances Outline:- Analysis of N* contribution to  p → K +  How does using a Genetic Algorithm help? How much can.
(Day 3).
Status of NLOjet++ for dijet angular distributions
The study of pentaquark states in the unitary chiral approach
Matteo Negrini Frascati, Jan 19, 2006
ppZZ4μ background process
Jim Marie Advisor: Richard Jones University of Connecticut
CP Violating TGCs Tim Barklow July 2, 2003.
Changyi Zhou (McGill University )
Unfolding Problem: A Machine Learning Approach
p0 life time analysis: general method, updates and preliminary result
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
A New Measurement of |Vus| from KTeV
Monte Carlo Simulation of Neutrino Mass Measurements
J/   analysis: preliminary results and status report
Study of excited baryons at BESII
First discovery of Double Cabbibo-Suppressed decay: Lc  pK+p- + a
Prospects for quarkonium studies at LHCb
e+e−→ J/ D(*)D(*) & ψ(4160) → DD
Study of e+e collisions with a hard initial state photon at BaBar
Search for (3770) non-DD-bar Decays
Unfolding with system identification
Recent BESII Hot Topics
The Q+ Pentaquark Search at HERMES Wolfgang Lorenzon Collaboration
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Observation of non-BBar decays of (4S)p+p- (1S, 2S)
Presentation transcript:

Partial Wave Analysis results from JETSET the Jetset experiment Gluonic Excitations Workshop Newport News, May 14-16, 2003 Partial Wave Analysis results from JETSET Richard Jones University of Connecticut representing the Jetset collaboration with members from Bari, CERN, Erlangen, Freiburg, Genova, Illinois, Jülich, Oslo, Uppsala the Jetset experiment PWA formalism and MC tests results from analysis of full data set

The Jetset Experiment Measures in-flight pbar annihilation: OZI-suppressed, may form glueball resonances in s-channel p f ? p f Morningstar et.al., LAT991004 R.T. Jones Newport News, May 14-16, 2003

Total cross section Complete data set from Jetset point N(ff) N(b.g.) 1 2 3 4 326 414 626 840 95 225 270 369 5 6 7 8 1005 1262 1782 1375 589 585 886 868 9 10 11 12 1318 1056 936 707 877 943 1592 1666 R.T. Jones Newport News, May 14-16, 2003

PWA Accounting J values of the waves included in the partial wave analysis. All waves up to J=4, L=4 in the final state were allowed. wave JPC L initial S initial L final S final 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 0-+ 0++ 1++ 2++ 2-+ 3++ 4-+ 4++ 1 2 3 4 5 1 1 2 4 3 1 2 R.T. Jones Newport News, May 14-16, 2003

We found 3 dominant waves PWA Procedure Getting started: Fit with all waves free gives full freedom to the fit -> definition of “good fit” errors on amplitudes are large, meaningless Reduce the set of allowed waves in search of a minimal set that gives a good description of the entire data set gives priority to an economical description adequacy judged in comparison with full fit require same set of waves for all mass bins We found 3 dominant waves all 2++ Method: 1. Group the data into mass bins with sufficient statistics 2. For each bin, try all waves one-by-one, keep best, repeat Sets agreed on 3 top waves. 3. Go back to beginning and put in waves two-by-two trying all pairs of waves together, then add one-by-one Sets chose same set of 3 waves as dominant. R.T. Jones Newport News, May 14-16, 2003

2 kinds: Ambiguities Essential ambiguities Statistical ambiguities correspond to invariances in angular distributions from PWA expansion continuous invariances : global phases (2) discrete invariances: undetermined signs (4) no others believed to exist for 2(V®2P) irreducible even in limit of good acceptance and high statistics Statistical ambiguities correspond to different angular distributions which cannot be discriminated given the available data discrete (different local maxima in likelihood) discovered by systematic numerical search reducible by good acceptance and high statistics relatively few in this data set R.T. Jones Newport News, May 14-16, 2003

Monte Carlo test Ingredients: 1 resonant wave, two non-resonant experimental acceptance through simulation same reconstruction, analysis as for real data R.T. Jones Newport News, May 14-16, 2003

Results of Monte Carlo test R.T. Jones Newport News, May 14-16, 2003

Monte Carlo test #2 include incoherent background uniform angular distribution for background not orthogonal to waves -- check for leakage R.T. Jones Newport News, May 14-16, 2003

Results of Monte Carlo test #2 R.T. Jones Newport News, May 14-16, 2003

PWA Results 3-wave fit identical to Monte Carlo test #2 simultaneous fit in mass and angular distributions ff cross section now corrected for acceptance based on measured angular distribution R.T. Jones Newport News, May 14-16, 2003

3-wave fit R.T. Jones Newport News, May 14-16, 2003

Possible Interpretation narrow peak seen in raw cross section PWA reveals 3 dominant waves in 2++ rapid phase motion seen in two waves as expected for a Breit-Wigner resonance R.T. Jones Newport News, May 14-16, 2003

Quality of the fit To check goodness of fit, use likelihood ratio test For large N, behaves like chi-square with n-n0 d.o.f. Define where L0 is the likelihood maximum over the full parameter space and L is the likelihood maximum over some restricted part. R.T. Jones Newport News, May 14-16, 2003

6-wave fit R.T. Jones Newport News, May 14-16, 2003

6-wave fit R.T. Jones Newport News, May 14-16, 2003

Total 2++ from 6-wave fit Some strength in 2++ has moved to 3++ No obvious narrow structure is visible in 2++ Phase motion seen does not correspond to a simple Breit-Wigner resonance Statistical errors do not justify a serious attempt to perform a multiple-pole fit R.T. Jones Newport News, May 14-16, 2003

BUT AND Conclusions PWA has been performed of the reaction 3 dominant waves were found, all 2++. Rapid phase motion seen in two waves consistent with a narrow 2++ resonance. The fit shows significant improvement if more waves are added, up to 6. Statistical errors do not permit a clear interpretation of 6-wave solution, but it does not favour a single narrow resonance. Possible interference between the ff and an underlying f0,f0 background should be taken into account. BUT AND R.T. Jones Newport News, May 14-16, 2003

5-wave fit R.T. Jones Newport News, May 14-16, 2003

5-wave fit R.T. Jones Newport News, May 14-16, 2003