The g 2^pExperiment - Thomas Jefferson National...

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The 𝑔2𝑝

ExperimentToby Badman

The University of New HampshireOn Behalf of the E08-027 Collaboration

Inclusive Electron Scattering

π‘‘πœŽ

𝑑Ω𝑑𝐸′= πœŽπ‘€π‘œπ‘‘π‘‘

1

𝜈𝐹2 π‘₯, 𝑄

2 +2

𝑀𝐹1 π‘₯, 𝑄

2 π‘‘π‘Žπ‘›2πœƒ

2

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Unpolarized nucleon structure functions.

ee’

P

Wπ›Ύβˆ—

Inclusive Electron Scattering

π‘‘πœŽ

𝑑Ω𝑑𝐸′= πœŽπ‘€π‘œπ‘‘π‘‘

1

𝜈𝐹2 π‘₯, 𝑄

2 +2

𝑀𝐹1 π‘₯, 𝑄

2 π‘‘π‘Žπ‘›2πœƒ

2+ 𝛾𝑔1 π‘₯, 𝑄

2 + 𝛿𝑔2(π‘₯, 𝑄2)

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Polarized nucleon spin structure functions.

ee’

P

W

Polarized target

Polarized π‘’βˆ’ beamπ›Ύβˆ—

Inclusive Electron Scattering

βˆ†πœŽβˆ₯ =𝑑2πœŽβ†‘β‡‘

π‘‘Ξ©π‘‘πΈβˆ’π‘‘2𝑑↓⇑

π‘‘Ξ©π‘‘πΈβˆ 𝛼𝑔1 π‘₯, 𝑄

2 βˆ’ 𝛽𝑔2 π‘₯, 𝑄2

βˆ†πœŽβŠ₯ =𝑑2πœŽβ†‘β‡’

π‘‘Ξ©π‘‘πΈβˆ’π‘‘2𝑑↓⇒

π‘‘Ξ©π‘‘πΈβˆ 𝛾𝑔1 π‘₯, 𝑄

2 + 𝛿𝑔2 π‘₯, 𝑄2

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Inclusive Electron Scattering

𝑔1 π‘₯, 𝑄2 ∝ βˆ†πœŽβˆ₯ + tan

πœƒ

2βˆ†πœŽβŠ₯

𝑔2 π‘₯, 𝑄2 ∝ βˆ’βˆ†πœŽβˆ₯ +

1 + 1 βˆ’ 𝑦 cos πœƒ

1 βˆ’ 𝑦 sin πœƒβˆ†πœŽβŠ₯

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β€’ βˆ†πœŽβˆ₯ is highly suppressed in the kinematic range where we are measuring 𝑔2 (2-8% of total contribution to 𝑔2).

β€’ For kinematic settings where we will not measure βˆ†πœŽβˆ₯, EG4 data will be combined with our βˆ†πœŽβŠ₯ data to calculate 𝑔2.

Motivation

β€’ Measure the proton structure function, 𝑔2, in the low 𝑄2 region for the first time.

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SLAC JLAB SANE

Motivation

β€’ Measure the proton structure function, 𝑔2, in the low 𝑄2 region for the first time.

β€’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low 𝑄2 region.

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Motivation

The 0π‘‘β„Ž moment of 𝑔2 should

satisfy (for all 𝑄2):

01𝑔2 π‘₯, 𝑄

2 𝑑π‘₯ = 0

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Brown: SLAC E155xRed: Hall C RSSBlack: Hall A E94-010Green: Hall A E97-110Blue: Hall A E01-012

β€’ Good agreement with existing Neutron data.

β€’ Some disagreement with existing proton data.

β€’ More proton data is needed.

Motivation

β€’ Measure the proton structure function, 𝑔2, in the low 𝑄2 region for the first time.

β€’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low 𝑄2 region.

β€’ Benchmark test of Chiral Perturbation Theory by extracting the generalized longitudinal-transverse spin polarizability.

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Spin Polarizability

𝛿𝐿𝑇 𝑄2 =

16𝛼𝑀2

𝑄6

0

π‘₯0

𝑑π‘₯ π‘₯2 𝑔1 π‘₯, 𝑄2 + 𝑔2 π‘₯, 𝑄

2

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β€’ Neutron data shows deviations from πœ’π‘ƒπ‘‡calculations.

β€’ No proton data yet!

Neutron

Motivation

β€’ Measure the proton structure function, 𝑔2, in the low 𝑄2 region for the first time.

β€’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low 𝑄2 region.

β€’ Benchmark test of Chiral Perturbation Theory by extracting the generalized longitudinal-transverse spin polarizability.

β€’ Improve calculations of Proton Hyperfine Splitting.

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Experimental Setup

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Continuous Electron Beam Accelerator Facility (CEBAF)β€’ Maximum Energy 12GeVβ€’ 200πœ‡π΄ currentβ€’ Electron polarization ~85%

Thomas Jefferson National LaboratoryNewport News, Virginia

You are here

Experimental Setup

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Beam Current

Monitors

Beam Rasters

Chicane

Beam Position Monitor

Scattering Chamber

Local Dump

Septum Magnet

High Resolution Spectrometers

β€’ New beamline equipment installed for low current running (<100nA)

β€’ Chicane installed for transverse target field requirements.

β€’ Rotatable 2.5T/5T scattering chamber.

β€’ Local dump and septum magnets

Kinematics and Projections

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0.02 < 𝑄2 < 0.2𝐺𝑒𝑉2

Beam Energy (GeV)

Target Field (T)

1.158 2.5

1.706 2.5

2.254 2.5

2.254 5.0

3.352 5.0

Kinematics and Projections

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LT Spin PolarizabilityBC Sum Integral

Analysis Progress

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Completedβ€’ Run DBβ€’ HRS Optics

β€’ Field Measurement Analysisβ€’ VDC t0 calibrationβ€’ Simulation Packageβ€’ Optics Reconstruction

β€’ Detector Calibrations/Efficienciesβ€’ Scalers

β€’ Helicity Decodingβ€’ BCM calibrationsβ€’ Deadtime calculations

β€’ Target Polarizationsβ€’ BPM calibrationsβ€’ Raster size calibration

In Progressβ€’ Packing fraction/dilution analysisβ€’ Elastic PBPt checkβ€’ Radiative correctionsβ€’ Acceptance study

Online Results

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Courtesy R. Zielinski

Online Results

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Summary

β€’ The 𝑔2𝑝

Experiment ran very successfully in spring, 2012.

β€’ New instrumentation and beam requirements (and fires) introduced many challenges to the running and analysis.

β€’ A first pass of production data is complete and analysis is well underway!

β€’ We hope to have offline asymmetries and cross-sections by spring of next year

β€’ 𝑔2 calculation shortly after, possibly by summer, 2015.

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E08-027 Collaboration

SpokespeopleAlexander CamsonneJ.P. ChenDon CrabbKarl Slifer

Post DocsKalyan AlladaEllie LongJames MaxwellVince SulkoskyJixie Zhang

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Graduate StudentsToby BadmanMelissa CummingsChao GuMin HuangJie LiuPengjia ZhuRyan Zielinski

Thank You!