Photoproduction of ϕ-meson by Using Linearly-Polarized Photons at Threshold Energies

Similar documents
Photoproduction of K 0 Σ + with CLAS

Measurement of Polarization Observables Pz, P s z and P c z in Double-Pion Photoproduction off the Proton

Search for New and Unusual Strangeonia States Using γp pφη with GlueX at Thomas Jefferson National Accelerator Facility

Vector-Meson Photoproduction

Measurement of the Polarization Observables. Spectrometer. I s and I c for γp p π + π using the CLAS. Charles Hanretty.

Photoproduction of vector mesons

The Beam-Helicity Asymmetry for γp pk + K and

The Determination of Beam Asymmetry from Double Pion Photoproduction

The x(1280) Meson in CLAS g11. Ryan Dickson Carnegie Mellon University May 31st, 2010

Vector Meson and Associated Strangeness Production Using a Linearly Polarized Photon Beam at Jefferson Lab

Strangeness photoproduction at the BGO-OD experiment

High-t Meson Photoproduction: Experimental Capabilities

Mukesh Saini. Florida State University, Tallahassee, FL. February 26, FSU Nuclear Physics Seminar. February 26

M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy. A Forward Photon Tagging Facility for CLAS12

DETERMINATION OF THE LINEAR POLARIZATION FOR THE HALL-B PHOTON BEAM AT JLAB

Experiments using polarized photon beam and polarized hydrogen-deuteride (HD) target

2.24 Simulation Study of K L Beam: K L Rates and Background Ilya Larin Department of Physics Old Dominion University Norfolk, VA 23529, U.S.A.

Hadron Spectroscopy at COMPASS

Light-Meson Spectroscopy at Jefferson Lab

in high statistics experiments at CLAS

Study of Excited Baryons with the Crystal-Barrel Detector at ELSA

Beam Asymmetry measurement in Pion Photoproduction on the neutron using CLAS

Kaon Photoproduction Results from CLAS

Hall-D Update. Eric Pooser. Joint Hall A/C Summer Collaboration Meeting 07/18/2015

Double polarization measurements with the Crystal Barrel/TAPS experiment at ELSA

Baryon Spectroscopy at ELSA

Strangeonia. Of the 22 expected resonances, only 7 are well identified. Strangeonia. η-η' h1 (1386) (1020) f2' (1525) f1 (1426) (1680)

Study of e + e annihilation to hadrons at low energies at BABAR

Overview of the LEPS facility Recent Results

CLEO Results From Υ Decays

Coherent Photoproduction of Proton-Antiproton Pairs on Deuterium

Beam-Helicity Asymmetry ƔP P K+K system

Light Baryon Spectroscopy using the CLAS Spectrometer at Jefferson Laboratory

Search for Gluonic Excitations with GlueX at Jefferson Lab

The Jefferson Lab 12 GeV Program

Threshold photoproduction of J/y with the GlueX experiment. Lubomir Pentchev Jefferson Lab for the GlueX collaboration

Recoil Polarisation Measurements in Meson Photoproduction

G13 Update. CLAS collaboration meeting

Cascade Spectroscopy at CLAS

Photoproduction of the f 1 (1285) Meson

Double Charm Baryon Studies in SELEX: Further Studies and Production Questions James Russ, Carnegie Mellon Outline

Baryon Spectroscopy at Jefferson Lab What have we learned about excited baryons?

Investigation of K0 + photoproduction with the CBELSA/TAPS experiment

Overview of recent HERMES results

Helicity Dependent Cross Sections in Meson Photoproduction off Quasi-Free Protons and Neutrons

N* and Y* baryon spectroscopy using high momentum pion beam (+ kaon beam) Hiroyuki Kamano (RCNP, Osaka U.)

Search for Pentaquarks at CLAS. in Photoproduction from Proton

HASPECT in action: CLAS12 analysis of

Studies of charmonium production in e + e - annihilation and B decays at BaBar

XVII International Conference on Hadron Spectroscopy and Structure - Hadron September, 2017 University of Salamanca, Salamanca, Spain

Timelike Compton Scattering

K 0 and Λ photoproduction using linearly polarized photons

Production and Searches for Cascade Baryons with CLAS

Properties of the Λ(1405) Measured at CLAS

Hall D & GlueX Update. Alex Barnes, University of Connecticut

Baryon Spectroscopy with Polarised Photon Beams at ELSA

LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration

Analysis of Lepton Pair Production at GlueX

Modifications of the D33(1700) resonance in the nuclear medium

CharmSpectroscopy from B factories

A search for baryon-number violating Λ ml decays using JLab

and ' Time-like Transition Form Factors from MAMI

Deeply Virtual Compton Scattering and Meson Production at JLab/CLAS

Probing Generalized Parton Distributions in Exclusive Processes with CLAS

Baryon Spectroscopy: Recent Results from the CBELSA/TAPS Experiment

The π 0 Lifetime Experiment and Future Plans at JLab

Moskov Amaryan Old Dominion University On behalf of the CLAS Collaboration

Facilities and Detectors for Baryon Physics

Measurement of the η-mass from the reaction γp pη in threshold region

Understanding Excited Baryon Resonances: Results from polarization experiments at CLAS

Charged Particle Identification in GLUEX

A Measurement of the Induced polarization of electro-produced Λ(1116) with CLAS

Measuring Form Factors and Structure Functions With CLAS

Search for exotic charmonium states

Hadron Physics with Real and Virtual Photons at JLab

Baryons 2016 International Conference on the Structure of Baryons May 16-20, Tallahassee, Florida G. Fedotov, R. Gothe, V. Burkert, and V.

GlueX Capabilities for Nuclear Photoproduction

Hunting for the Nucleon Resonances by Using Kaon Photoproduction

Recent Results on Spectroscopy from COMPASS

Meson Physics with Crystal Ball at MAMI

Selected results in hadronic final state in DIS at HERA

Cross Section of Exclusive π Electro-production from Neutron. Jixie Zhang (CLAS Collaboration) Old Dominion University Sep. 2009

Deeply Virtual Compton Scattering off 4. He: New results and future perspectives

Production cross sections of strange and charmed baryons at Belle

Overview and Status of Measurements of F 3π at COMPASS

Charm and Beauty Structure of the proton

Sven Schumann. DPG Spring Meeting

Simulation of X(3872) Resonance Scan Using the PandaRoot Framework 1

Recent Heavy Flavors results from Tevatron. Aleksei Popov (Institute for High Energy Physics, Protvino) on behalf of the CDF and DØ Collaborations

The D-wave to S-wave amplitude ratio for b 1 (1235) ωπ

Hans-Jürgen Arends Mainz University

Proton Form Factor Puzzle and the CLAS Two-Photon Exchange Experiment

Meson spectroscopy at CLAS and CLAS12: the present and the future. Raffaella De Vita INFN Genova for the CLAS Collaboration

D0 and D+ Hadronic Decays at CLEO

Recent results on exclusive hadronic cross sections measurements with the BABAR detector

Study of the decays at Wasa-at-COSY. Elisabetta Prencipe on behalf of the Wasa Collaboration MesonNet Workshop, 17th -19th June 2013, Praha

Current Status of Hadronic Physics with at

A Comprehensive Study of the Radiative Decay of J/ψ and ψ(2s) to Pseudoscalar Meson Pairs and Search for Glueballs

Charmonium(-like) and Bottomonium(-like) States Results from Belle and BaBar

arxiv: v1 [nucl-ex] 9 Jul 2013

Transcription:

Photoproduction of ϕ-meson by Using Linearly-Polarized Photons at Threshold Energies Julian Salamanca, Philip L Cole and the CLAS Collaboration CLAS Collaboration Meeting Newport News, VA June 12, 2009

Outline Motivation OZI evading/respecting VMD (Vector Meson Dominance) Spin Density Matrix Elements ϕ-meson Photoproduction CEBAF (Continuous Electron Beam Accelerator Facility ) Coherent Bremsstrahlung Facility at CLAS (CEBAF Large Acceptance Spectrometer) Event Selection Background Subtraction Results for the 1.9 GeV Coherent-Edge Results for the 2.1 GeV Coherent-Edge

OZI evading/respecting process Okubo Zweig Iizuka rule: In strong interaction processes where final states can only be reached via quarkantiquark annihilation are suppressed. You cannot cut gluon lines in the OZI picture. ( 49.2 ± 0.6) % ( 34 ± 0.5) % Experimentally this decay mode is: (15.3 ± 0.4)% ~84% of the Φ decay is OZI respecting.

VMD

Previous Measurements J. Ballam, G. B. Chadwick et al., Phys. Rev. D 7 3150 (1972).

Previous Measurements Spring-8 used a beam of linearly polarized photons (forward direction t <0.4 GeV 2) T. Mibe, Measurement of φ meson photoproduction near production threshold with linearly polarized photons, PhD Thesis, Osaka University, Japan (2004), unpublished. T. Mibe et al., Phys. Rev. Lett. 95, 182001 (2005).

The Decay Angular Distribution Spin Density Matrix Elements Linearly polarization gives access to six more density matrix elements *Those are calculated in φ rest frame (Helicity Frame)

Spin Density Matrix Elements IF VMD: Density matrix elements should be equal to ZERO but ρ11-1 and Im{ρ21-1} ρ11-1, Im{ρ21-1} = (1/2, -1/2 : Pomeron) ρ11-1, Im{ρ21-1} = (-1/2, 1/2 : Meson)

ϕ Photoproduction: g8b experiment Linearly Polarized Photon Beam p(π,η,η,ρ,ω,ϕ), KΛ Target: Hydrogen

The Coherent Bremsstrahlung Facility at CLAS Requirements for Coherent Bremsstrahlung Low emittance, stable beam High quality thin crystal Collimation < 0.5 characteristic angle Photon Tagger Goniometer and Diamond 23m Pair Spectrometer CLAS detector LH2 target Active collimator Polarimeter Experiments with Linearly Polarized Photons at CLAS Beam Profiler

The Coherent Bremsstrahlung Facility at CLAS Diamond Goniometer, Experiments with Linearly Polarized Washington Photons at CLAS George University

Linearly Polarized Photons i. e. Coherent Peak at 2.1 GeV Mean polarization estimated to be ~70% from comparison with the coherent bremsstrahlung calculation* * A. Natter. http://www.pit.physik.uni-tuebingen.de/grabmayr/software/brems/brems-analytic.html

Event Selection γ p pϕ pk+kmode: pk+(x) pk+(k-) 1.9GeV CohEdge 2.1GeV CohEdge

Event Selection i.e. 2.1GeV CohEdge Quality flags: TAGR status = 7 or 15 EVNT DC status > 0 EC status > 0 Status > 0 Loose cuts on p and K + masses. Applied cuts were 0.8 < mp < 1.2 GeV and 0.3 < mk + < 0.7 GeV.

Event Selection Timing cuts base on proton vertex time

Event Selection 1.9GeV CohEdge 2.1eV CohEdge Energy cut: 1.68 to 1.92 GeV 1.88 to 2.102 GeV

Event Selection K missing mass cut A 5-sigma cut on the K missing mass was applied by using a Gaussian function + 2nd polynomial. i.e. PERP 1.9 GeV CohEdge i.e. PARA 2.1 GeV CohEdge

Event Selection 1.9 GeV CohEdge i.e. PERP 2.1 GeV CohEdge i.e.para π + background subtraction

Event Selection Time difference between p and K+ vertex times. It seems the event selection we made was not enough to get rid of the π + background. The tails coming down from a maximum located around -4ns ( 1.9 GeV CohEdge ) and -3ns (2.1 GeV CohEdge data ) seem to be fully misidentified kaons. Applying the tp tπ+ < -4 ns (-3 ns) condition improves our results. Time difference between p and π + vertex times. 1.9 GeV CohEdge 2.1 GeV CohEdge

Energy-Balance check : Minitial Mfinal ~ 0 i.e. 1.9 GeV CohEdge Event Selection -0.01 < Minitial Mfinal < 0.003 GeV PARA PARA No cut PARA With cut PERP PERP PERP PARA No cut With cut

Φ-meson reconstruction was fitted by a Breit-Wigner convoluted with a Gaussian + 2nd order polynomial (We fix ГΦ = 4.26 MeV from PDG) PARA Event Selection PERP 1.9 GeV Coh Edge 2.1 GeV Coh Edge

Probabilistic Event Weighting* Q-factor = Fs/(Fs+Fb) Fs (Signal): Voigtian Fb (Background): 2nd order polynomial Background Subtraction i.e 2.1 GeV Coh Edge ---- Q-Factor ---- 1 - Q-Factor * M. Williams, M. Bellis and C.A. Meyer arxiv: 0804.3382v1 MΦ

SDME parametrization.

Results PRELIMINARY 1.9 GeV CohEdge PRELIMINARY 2.1 GeV CohEdge

Results PRELIMINARY 1.9 GeV CohEdge PRELIMINARY 2.1 GeV CohEdge

Momentum Corrections? i.e. 1.9 GeV CohEdge i.e. 2.1 GeV CohEdge

Conclusions Polarization ~70% Over 14000 ϕ-meson events were analyzed. Extract Spin Density Matrix Elements (SDMEs) Double check on Polarization calculation Study of systematic errors Compare to Spring-8[1] data as well as J. Ballam et al. Write up!!! [1] T. Mibe et al., Phys. Rev. Lett. 95, 182001 (2005). [2] J. Ballam, G. B. Chadwick, et al., Phys. Rev. D 7 3150 (1972).

g8 history so far

g8b (6/20 9/01/05) Tagged and Collimated γ beam in Hall B for beam-asymmetry studies for the reactions: γp Coh. Peak 1.3 GeV 1.5 GeV 1.7 GeV 1.9 GeV 2.1 GeV Amorphous p(π,η,ρ,ω,φ),kλ good evts (1.4 Billion) (2.0 Billion) (1.8 Billion) (1.2 Billion) (0.9 Billion) (1.8 Billion) Photon Polarization exceeds 90% in the peak ρ0 at low t (< 0.30 GeV2) Thanks!!!