Search for Gluonic Excitations in Hadrons with GlueX Hadron 2011 - - PowerPoint PPT Presentation

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Search for Gluonic Excitations in Hadrons with GlueX Hadron 2011 - - PowerPoint PPT Presentation

Introduction Detector Search for Gluonic Excitations in Hadrons with GlueX Hadron 2011 Igor Senderovich June 16, 2011 Igor Senderovich Search for Gluonic Excitations in Hadrons with GlueX 1 Introduction Physics Motivation Detector


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Introduction Detector

Search for Gluonic Excitations in Hadrons with GlueX

Hadron 2011 Igor Senderovich June 16, 2011

Igor Senderovich Search for Gluonic Excitations in Hadrons with GlueX 1

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Introduction Detector Physics Motivation Production Approach

Outline

Introduction Physics Motivation Production Approach Detector Detector Overview Trigger and Readout

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Introduction Detector Physics Motivation Production Approach

Physics Motivation Can we probe the gluonic field in hadrons directly?

◮ hybrid mesons (i.e. with gluonic excitation)

Figure: Lattice QCD mass predictions as a function of pion

  • mass. (J. Dudek et al., 2010)

Other physics:

◮ precision measurement of

Γ(η → γγ) via Primakoff effect†

◮ general

light-quark spectroscopy, e.g.

◮ excited vector

mesons poorly understood

◮ strange sector

analogs of X, Y, Z mesons

◮ understand the Ξ spectrum ◮ inverse DVCS ◮ production near charm threshold ◮ hadronization in the nuclear

medium

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†approved

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Introduction Detector Physics Motivation Production Approach

Meson Quantum Numbers

Consider the qq system and its JP C quantum numbers. Since:

◮ S = 0, 1 and L = 0, 1, 2, . . . =

⇒ J = L − 1, L, L + 1

◮ P = (−1)L+1 and C = (−1)L+S

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Introduction Detector Physics Motivation Production Approach

Meson Quantum Numbers

Consider the qq system and its JP C quantum numbers. Since:

◮ S = 0, 1 and L = 0, 1, 2, . . . =

⇒ J = L − 1, L, L + 1

◮ P = (−1)L+1 and C = (−1)L+S

∴ qq quantum numbers: J −− ++ −+ +− 0++ 0−+ 1 1−− 1++ 1+− 2 2−− 2++ 2−+ 3 3−− 3++ 3+− 4 4−− 4++ 4−+ 5 5−− 5++ 5+−

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Introduction Detector Physics Motivation Production Approach

Meson Quantum Numbers

Consider the qq system and its JP C quantum numbers. Since:

◮ S = 0, 1 and L = 0, 1, 2, . . . =

⇒ J = L − 1, L, L + 1

◮ P = (−1)L+1 and C = (−1)L+S

∴ qq quantum numbers: “exotic” quantum numbers: J −− ++ −+ +− 0−− 0++ 0−+ 0+− 1 1−− 1++ 1−+ 1+− 2 2−− 2++ 2−+ 2+− 3 3−− 3++ 3−+ 3+− 4 4−− 4++ 4−+ 4+− 5 5−− 5++ 5−+ 5+−

◮ Exotic states =

⇒ unambiguous signature of new degrees of freedom

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Introduction Detector Physics Motivation Production Approach

Exotic States: Experimental Evidence

The following are some tentative observations of possible exotic states thus far:1

State Mass (GeV) Width (GeV) Prod. Decays Experiments π1(1400) 1.351 ± 0.03 0.313 ± 0.040 π−p, ¯ pn π−η,π0η E852, CBAR π1(1600) 1.662 ± 0.015 0.234 ± 0.050 π−p, ¯ pp η′π, b1π, f1π, ρπ E852, CBAR, COMPASS, VES π1(2015) 2.01 ± 0.03 0.28 ± 0.05 π−p b1π,f1π E852

1masses and widths from PDG

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Introduction Detector Physics Motivation Production Approach

Production Method

Data so far: (mostly) π beam prod. ⇐

= exotic hybrid prod. suppressed? A possible argument: the spin flip needed for exotic q.n. is suppressed. Proposal: use S = 1 beam → photons! Lowest-lying hybrids (flux-tube model): N N X π N N X γ π beam (S = 0) γ beam (S = 1) 0−− 0++ 0−+ 0+− 1−− 1++ 1−+ 1+− 2−− 2++ 2−+ 2+− γ beam source: Coherent Bremsstrahlung in diamond

◮ 9 GeV, 40% polarization fraction ◮ 108γ/s with ∼ 2 µA beam current ◮ collimation 75 m downstream ◮ 8 MeV/counter tagging with high efficiency

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Introduction Detector Detector Overview Trigger and Readout

12 GeV upgrade

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Introduction Detector Detector Overview Trigger and Readout

12 GeV upgrade

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Introduction Detector Detector Overview Trigger and Readout

12 GeV upgrade

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Introduction Detector Detector Overview Trigger and Readout

Hall Construction

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Introduction Detector Detector Overview Trigger and Readout

Hall Construction

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Introduction Detector Detector Overview Trigger and Readout

Detector Overview

  • 185cm

30cm-Target 560cm 48cm 126.4 118.1

  • 342cm
  • C

L

  • 14.7

10.8

  • tracking system

calorimetry time of flight solenoid future PID

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◮ 2.2 T solenoid ◮ 30 cm LH2

target

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Introduction Detector Detector Overview Trigger and Readout

Barrel Calorimeter (BCAL)

Sampling (10%) SpaCal

Design based on KLOE Emcal:

◮ 40 MeV − 3.5 GeV range ◮ 11◦ < θ < 120◦ coverage ◮ 191 Sci/Pb layers → 15.5 X0 ◮ σE/E = 5.54/

√ E ⊕ 1.6%

◮ σz = 5 mm ◮ σ∆t/2 = 70 ps/

√ E

◮ +5 ◦C-stabilized Hamamatsu

SiPM readout Role:

◮ γ, π0, η reconstruction ◮ PID input through: energy,

dE/dx, time of flight

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Introduction Detector Detector Overview Trigger and Readout

Barrel Calorimeter (BCAL)

Sampling (10%) SpaCal

Design based on KLOE Emcal:

◮ 40 MeV − 3.5 GeV range ◮ 11◦ < θ < 120◦ coverage ◮ 191 Sci/Pb layers → 15.5 X0 ◮ σE/E = 5.54/

√ E ⊕ 1.6%

◮ σz = 5 mm ◮ σ∆t/2 = 70 ps/

√ E

◮ +5 ◦C-stabilized Hamamatsu

SiPM readout Role:

◮ γ, π0, η reconstruction ◮ PID input through: energy,

dE/dx, time of flight

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TOF

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Introduction Detector Detector Overview Trigger and Readout

Forward Calorimeter (FCAL)

Lead Glass Calorimeter

◮ 2◦ < θ < 11◦ coverage ◮ 2800 F8-00 Pb-glass blocks:

4 × 4 × 45 cm

◮ FEU 84-3 PMT readout ◮ σE/E = 5.7/

√ E ⊕ 1.6%

◮ σr = 5 − 6 mm ◮ σt < 150 ps

using algorithms on FPGA

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Introduction Detector Detector Overview Trigger and Readout

Central Drift Chamber (CDC)

Staw Tube Drift Chamber

◮ 3522 aluminized mylar straw

tubes, 1.6 cm dia.

◮ 12 axial, 16 (6◦) stereo layers ◮ dE/dx for π,K, p < 450 MeV/c ◮ σr = 150 µm, σz = 1.5 mm ◮ σp/p = 1.5 − 3% ◮ 6◦ < θ < 165◦ coverage

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Introduction Detector Detector Overview Trigger and Readout

Forward Drift Chamber

Cathode Strip Design:

◮ 4 packages × 6 planes/package × 96 wires/plane = 2304 wires ◮ 4 packages × 12 planes/package × 216 strips/plane= 10368 strips

Figure: Cathode readout, redundancy and angular shifts to reduce ghosting. Next layer

  • ffset by 60◦

◮ 1 cm sense wire pitch ◮ 0.5 cm cathode plane pitch ◮ σx,y = 200 µm ◮ 1◦ < θ < 30◦ coverage

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Introduction Detector Detector Overview Trigger and Readout

Time of Flight Wall and Start Counter

Time of Flight Wall

◮ cross-hatched scintillator paddles ◮ 2.5 cm thick, 6 cm wide ◮ double-sided readout ◮ goal: 100 ps = (σ0 = 80 ps) ⊕ (σT DC = 60 ps)

Demonstrated so far: 110 ps

Start Counter: beam bunch ID

◮ 40 scintillators with cooled SiPM readout ◮ σt optimization in progress: material/resolution

trade-off

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Introduction Detector Detector Overview Trigger and Readout

Electronics & Software

Fully pipelined front-end electronics

◮ VMEx64/VXS startards ◮ fADC: 12 bit, 8 µs buffer with FPGA-based algorithms. Version:

◮ 250 MHz, 16 channel ◮ 125 MHz, 72 channel

◮ F1TDC: 3.9 µs buffer (3 µs trigger latency expected)

◮ 60 ps resolution, 32 channel ◮ 120 ps resolution, 64 channel

◮ ∼ 3 GB/s DAQ rate, ∼ 300 MB/s to tape → L3 computer farm essential

Software: significant efforts in parallelization

  • 1. vectorized operations on CPU (SIMD etc.)
  • 2. GPU for PWA fits, tracking?
  • 3. fully-multithreaded reconstruction/analysis code, on-demand

reconstruction

  • 4. integration of beowulf clusters and collaboration with Open Science Grid

(OSG)

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Introduction Detector Detector Overview Trigger and Readout

Trigger

10

7γ/s

10

8γ/s

~20kHz L3 Tape L1 low-lumi. high-lumi.

Goal: high-multiplicity, minimum-bias events Eγ > 8.4 GeV

  • 1. commissioning, warm-up at 107 γ/s
  • 2. full hardonic rate: 108 γ/s

∴ photo-production: 360 kHz

Alogorithm: require:

  • 1. track multiplicity
  • 2. energy minimum:

EBCAL = A + B · EF CAL

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Introduction Detector Detector Overview Trigger and Readout

Trigger

10

7γ/s

10

8γ/s

~20kHz L3 Tape L1 low-lumi. high-lumi.

Goal: high-multiplicity, minimum-bias events Eγ > 8.4 GeV

  • 1. commissioning, warm-up at 107 γ/s
  • 2. full hardonic rate: 108 γ/s

∴ photo-production: 360 kHz

Alogorithm: require:

  • 1. track multiplicity
  • 2. energy minimum:

EBCAL = A + B · EF CAL

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Introduction Detector Detector Overview Trigger and Readout

Trigger

10

7γ/s

10

8γ/s

~20kHz L3 Tape L1 low-lumi. high-lumi.

Goal: high-multiplicity, minimum-bias events Eγ > 8.4 GeV

  • 1. commissioning, warm-up at 107 γ/s
  • 2. full hardonic rate: 108 γ/s

∴ photo-production: 360 kHz

Alogorithm: require:

  • 1. track multiplicity
  • 2. energy minimum:

EBCAL = A + B · EF CAL

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Introduction Detector Detector Overview Trigger and Readout

Acceptance relative to E852

Goal set forth: high and uniform acceptance

Figure: Comparative acceptance plots in a sample channel: high and uniform acceptance in invariant mass and Gottfried-Jackson frame angles.

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Introduction Detector Detector Overview Trigger and Readout

Summary

GlueX: an imperative new search

◮ mesons with excited gluonic degrees of freedom

◮ an important test of QCD ◮ understanding confinement

◮ vast new source of photo-production data

Fitness for its mission:

◮ linearly polarized photon beam ◮ high statistics with minimum-bias trigger ◮ hermetic detector → proper PWA ◮ construction on schedule, transition to installation ◮ beam in 2014 ◮ ...but plenty to do and with many openings for collaborators!

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Introduction Detector Detector Overview Trigger and Readout

Backup Slides

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Introduction Detector Detector Overview Trigger and Readout

Coherent Bremsstrahlung

Coherent scattering of e− on a crystal lattice.

  • r

quasi-Compton scattering from virtual photons in the crystal reciprocal lattice Result: bremsstrahlung spectrum enhancement with polarized γ peaks Issues: smearing from e− multiple scattering Experimental Implementation: diamond thinned to 20 µm to reduce multiple scattering

◮ 40% pol. frac. under 9 GeV peak ◮ 108γ/s with ∼ 2 µA beam current ◮ collimation with long lever arm (75 m

downstream) to filter out widely distributed incoherent photons.

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Introduction Detector Detector Overview Trigger and Readout

Beamline

12 GeV e

− beam

to dump 0.3 GeV 9 GeV broad-band hodoscope fine-resolution "microscope" diamond radiator

  • quad. magnet

dipole magnet photon beam 1 . 5 T f i e l d x z y

Figure: Schematic of optics in the Tagger Hall.

◮ Broad-band hodoscope

◮ γ-spectrum measured 3 − 11.7 GeV ◮ tagging 9 − 11.7 GeV ◮ 30 MeV/counter

◮ Fine-resolution hodoscope (“microscope”)

◮ tagging 8.3 − 9.1 GeV ◮ 8 MeV/counter ◮ vertical collimation for tagging efficiency

improvement

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Introduction Detector Detector Overview Trigger and Readout

Trigger

10

7γ/s

10

8γ/s

~20kHz L3 Tape L1 low-lumi. high-lumi.

Goal: high-multiplicity, minimum-bias events Eγ > 8.4 GeV

  • 1. commissioning, warm-up at 107 γ/s
  • 2. full hardonic rate: 108 γ/s

∴ photo-production: 360 kHz

Track multiplicity + energy requirement: EBCAL = A + B ˙ EF CAL

Figure: a distinct, low-end peak in energy distributions = ⇒ clear cut!

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Introduction Detector Detector Overview Trigger and Readout

Trigger Cut Effects

Result:

◮ low-energy hadronic rate cut

with good yield in area of interest

◮ rate after L1 @ 108 γ/s:

∼ 150 kHz < 200 kHz limit Checking some signal channels:

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