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The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014
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The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

Dec 27, 2015

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Page 1: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

The GlueX Experiment in Hall-D

Curtis A. MeyerGlueX Spokesperson

October 3, 2014

Page 2: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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The Long Road to Now• Jul. 1997 – Workshop at Indiana University• Dec. 1999 – External Project Review• Apr. 2004 – Critical Decision 0• Oct. 2004 – External Detector Review• Oct. 2008 – Critical Decision 3• Apr. 2009 – Hall-D Complex Ground Breaking• Jan. 2012 – Beneficial Occupancy of Hall D• May 2014 – 10.5 GeV electron beam to tagger dump.

• Oct. 2014 – Photon beam to GlueX.• Apr. 2015 – Engineering/Physics Running with GlueX.• Sep. 2015 – Physics Running with GlueX!

10/3/14

18 Years

Page 3: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Atoms are electricallyneutral: a charge and an anti-charge ( + - ).

The rules that govern how the quarks froze out into hadrons are given by QCD.

Quarks have colorcharge: red, blue andgreen. Antiquarkshave anticolors: cyan, yellow and magenta.

Hadrons are color neutral (white),red-cyan, blue-yellow, green-magentaor red-blue-green, cyan-yellow-magenta.

Quantum Chromo Dynamics

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Page 4: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Flux

tube

forms

between

qq

Color Field: Because of self interaction, confining flux tubes form between static color charges

Confinement arises from flux tubes and their excitation leads to a new spectrum of mesons

Quantum Chromo Dynamics

Page 5: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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The QCD Potential

linear potential

ground-state flux-tube m=0

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Page 6: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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The QCD Potential

linear potential

ground-state flux-tube m=0

Excited gluonic field

Gluonic Excitations provide anexperimental measurement of the excited QCD potential.

Observations of the nonets on the excited potentials are the best experimental signal of gluonic excitations.

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Page 7: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Quantum Chromo Dynamics

10/3/14

QCD describes the interactions of quarks and gluons and should predict the spectrum of bound-state baryons ( ) and mesons ( ).

There should also be mesons in which the gluonic field contributes directly to the JPC quantum numbers of the states --- hybrid mesons. Some are expected to have ``exotic’’ quantum numbers.

Lattice QCD calculation of the light-quark meson spectrum

Normal QN

Exotic QN

2.0GeV

Several nonets predicted

0+- 2+-1-+

2.5Gev

Page 8: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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QCD Exotics

p1 IG(JPC)=1-(1-+)

h’1 IG(JPC)=0+(1-+)

h1 IG(JPC)=0+(1-+)

K1 IG(JPC)= ½ (1-)

We expect 5 nonets of exotic-quantum-number mesons:

1 nonet of 0+- exotic mesons2 nonets of 1-+ exotic mesons2 nonets of 2+- exotic mesons

Lattice shows two nonets here.

Experimental evidence exists for p1 states.

3 types of quarks: up, down and strange3 types of anti-quarks:9 quark-antiquark pairs == nonet

Page 9: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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The GlueX Experiment

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Page 10: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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This technique provides requisite energy, flux and

polarization

electrons in

Linearly polarizedphotons out

spectrometer

20 mm thick Diamond crystal

flu

x

photon energy (GeV)

12 GeV electrons

collimated

Incoherent &coherent spectrum

tagged

with 0.1% resolution

40%polarization

in peak

Coherent Bremsstrahlung

Page 11: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Physics in

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8.4-9.0 GeV linearly polarized photons from 12 GeV electrons in a thin diamond wafer

Charged particle tracking + timing and photon detection in a 2T magnetic field.

Fully reconstruct final states

• All of these channels have been studied in Monte Carlo to understand the acceptance.

• These studies have been used to ``stress’’ our offline reconstruction software.

Page 12: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Summary• We are excited to have the GlueX/Hall-D

photoproduction programs starting very soon.

• We anticipate an exciting meson program over the next decade.

• When we are done, we hope that we have the answer to: ``Where are the QCD states with static glue?’’

10/3/14

Page 13: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Kaons do not have exotic QN’s

Expected Decay Modes 1 , b1 , f1, ’ph , a1

1 hf2,a2,hf1, ’h ,(1300), a1, 1’ K*K, K1(1270)K, K1(1270)K , ’h

b2 a2, rh, f1 , r a1, h1, b1hh2 b1,, f1wh’2 K1(1270)K, K1(1270)K, K2

*Kf, f1f

b0 (1300) , h1, f1r, b1hh0 b1 , h1h’0 K1(1270) , K (1460)K K, h1

Early Reach With Statistics Hard

Page 14: The GlueX Experiment in Hall-D Curtis A. Meyer GlueX Spokesperson October 3, 2014.

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Initial exotic hybrid searches

GlueX Physics Analysis

10/3/14

Physics reactions of interest:

Understand the detector

Strange Baryons Activity in the physics working group has shifted to physics analysis.

GlueX ready to do physics, analyses being worked out in advance using the full suite of GlueX/Hall-D software and data from large-scale data challenges.

Other Physics Interestsh Decaysh PrimakovJ/ y Production…