Post on 26-Feb-2019
The π2π
ExperimentToby Badman
The University of New HampshireOn Behalf of the E08-027 Collaboration
Inclusive Electron Scattering
ππ
πΞ©ππΈβ²= ππππ‘π‘
1
ππΉ2 π₯, π
2 +2
ππΉ1 π₯, π
2 π‘ππ2π
2
Toby Badman DNP 2014 2
Unpolarized nucleon structure functions.
eeβ
P
WπΎβ
Inclusive Electron Scattering
ππ
πΞ©ππΈβ²= ππππ‘π‘
1
ππΉ2 π₯, π
2 +2
ππΉ1 π₯, π
2 π‘ππ2π
2+ πΎπ1 π₯, π
2 + πΏπ2(π₯, π2)
Toby Badman DNP 2014 3
Polarized nucleon spin structure functions.
eeβ
P
W
Polarized target
Polarized πβ beamπΎβ
Inclusive Electron Scattering
βπβ₯ =π2πββ
πΞ©ππΈβπ2πββ
πΞ©ππΈβ πΌπ1 π₯, π
2 β π½π2 π₯, π2
βπβ₯ =π2πββ
πΞ©ππΈβπ2πββ
πΞ©ππΈβ πΎπ1 π₯, π
2 + πΏπ2 π₯, π2
Toby Badman DNP 2014 4
Inclusive Electron Scattering
π1 π₯, π2 β βπβ₯ + tan
π
2βπβ₯
π2 π₯, π2 β ββπβ₯ +
1 + 1 β π¦ cos π
1 β π¦ sin πβπβ₯
Toby Badman DNP 2014 5
β’ βπβ₯ is highly suppressed in the kinematic range where we are measuring π2 (2-8% of total contribution to π2).
β’ For kinematic settings where we will not measure βπβ₯, EG4 data will be combined with our βπβ₯ data to calculate π2.
Motivation
β’ Measure the proton structure function, π2, in the low π2 region for the first time.
Toby Badman DNP 2014 6
SLAC JLAB SANE
Motivation
β’ Measure the proton structure function, π2, in the low π2 region for the first time.
β’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low π2 region.
Toby Badman DNP 2014 7
Motivation
The 0π‘β moment of π2 should
satisfy (for all π2):
01π2 π₯, π
2 ππ₯ = 0
Toby Badman DNP 2014 8
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, π2, in the low π2 region for the first time.
β’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low π2 region.
β’ Benchmark test of Chiral Perturbation Theory by extracting the generalized longitudinal-transverse spin polarizability.
Toby Badman DNP 2014 9
Spin Polarizability
πΏπΏπ π2 =
16πΌπ2
π6
0
π₯0
ππ₯ π₯2 π1 π₯, π2 + π2 π₯, π
2
Toby Badman DNP 2014 10
β’ Neutron data shows deviations from πππcalculations.
β’ No proton data yet!
Neutron
Motivation
β’ Measure the proton structure function, π2, in the low π2 region for the first time.
β’ Provides a unique opportunity to test the Burkhardt-Cottingham Sum Rule in the low π2 region.
β’ Benchmark test of Chiral Perturbation Theory by extracting the generalized longitudinal-transverse spin polarizability.
β’ Improve calculations of Proton Hyperfine Splitting.
Toby Badman DNP 2014 11
Experimental Setup
Toby Badman DNP 2014 12
Continuous Electron Beam Accelerator Facility (CEBAF)β’ Maximum Energy 12GeVβ’ 200ππ΄ currentβ’ Electron polarization ~85%
Thomas Jefferson National LaboratoryNewport News, Virginia
You are here
Experimental Setup
Toby Badman DNP 2014 13
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
Toby Badman DNP 2014 14
0.02 < π2 < 0.2πΊππ2
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
Toby Badman DNP 2014 15
LT Spin PolarizabilityBC Sum Integral
Analysis Progress
Toby Badman DNP 2014 16
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
Toby Badman DNP 2014 17
Courtesy R. Zielinski
Online Results
Toby Badman DNP 2014 18
Summary
β’ The π2π
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’ π2 calculation shortly after, possibly by summer, 2015.
Toby Badman DNP 2014 19
E08-027 Collaboration
SpokespeopleAlexander CamsonneJ.P. ChenDon CrabbKarl Slifer
Post DocsKalyan AlladaEllie LongJames MaxwellVince SulkoskyJixie Zhang
Toby Badman DNP 2014 20
Graduate StudentsToby BadmanMelissa CummingsChao GuMin HuangJie LiuPengjia ZhuRyan Zielinski
Thank You!