![Page 1: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/1.jpg)
POETIC 2012Indiana University
From JLab12 to EIC
R. D. McKeown
12 GeV CEBAF
![Page 2: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/2.jpg)
2
Wpu(x,k
T,r ) Wigner distributions
d2kT
PDFs f1
u(x), .. h1u(x)
d3r
TMD PDFs f1
u(x,kT), .. h1u(x,kT)
3D imaging
6D Dist.
Form FactorsGE(Q2), GM(Q2)
d2rT
dx &Fourier Transformation
1D
Unified View of Nucleon Structure
GPDs/IPDs
d2kT drz
![Page 3: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/3.jpg)
3
Extraction of GPD’s
t
hard vertices
A =Ds2s
s+ - s-
s+ + s- =
Unpolarized beam, transverse target:
DsUT~ sinf{k(F2H – F1E)}df E( ,x t)
DsLU~ sinf{F1H+ ξ(F1+F2)H+kF2E}df~
Polarized beam, unpolarized target:
H(x,t)
ξ=xB/(2-xB)
Unpolarized beam, longitudinal target:
DsUL~ sinf{F1H+ξ(F1+F2)(H+ξ/(1+ξ)E)}df~ H(x,t)
~
Cleanest process: Deeply Virtual Compton Scattering
![Page 4: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/4.jpg)
4
DVCS beam asymmetry at 12 GeV CLAS12
ep epg
High luminosity and large acceptance allows wide coverage in Q2 < 8 GeV2, xB< 0.65, andt< 1.5GeV2
sinφ moment of ALU
![Page 5: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/5.jpg)
5
SIDIS Electroproduction of Pions
• Separate Sivers and Collins effects
• Sivers angle, effect in distribution function: (fh-fs)
• Collins angle, effect in fragmentation function: (fh+fs)
Scattering Plane
target angle
hadron angle
• Previous data from HERMES,COMPASS
• New landscape of TMD distributions
• Access to orbital angular momentum
![Page 6: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/6.jpg)
6
SoLID Transversity Projected Data
• Total 1400 bins in x, Q2, PT and z for 11/8.8 GeV beam.
• z ranges from 0.3 ~ 0.7, only one z and Q2 bin of 11/8.8 GeV is shown here. π+ projections are shown, similar to the π- .
![Page 7: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/7.jpg)
7
Quark Angular Momentum
7
→ Access to quark orbital angularmomentum
![Page 8: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/8.jpg)
8
Parity Violating Electron Scattering
8
![Page 9: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/9.jpg)
9
12 GeV
• With 12 GeV we study mostly the valence quark component
• An EIC aims to study gluon dominated matter.
Into the “sea”: EIC
mEIC
EIC
![Page 10: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/10.jpg)
10
![Page 11: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/11.jpg)
11
TMD studies at EIC
10 fb-1 @ each s
(from EIC White Paper)
![Page 12: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/12.jpg)
12
Extending Sivers Tomography
A. Prokudin
![Page 13: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/13.jpg)
13
Longitudinal Spin - DG
10 fb-1 – Stage 1
(from EIC White Paper)
![Page 14: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/14.jpg)
14
Gluon Tomography
DV J/ Y Production (from EIC White Paper)
![Page 15: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/15.jpg)
15
Precision Tests of the Standard Model
200 fb-1
![Page 16: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/16.jpg)
16
MEIC Design Report
• Web posting imminent
• Stable design for 3 years
![Page 17: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/17.jpg)
17
Medium Energy EIC@JLab
JLab Concept
Initial configuration (MEIC):• 3-11 GeV on 20-100 GeV ep/eA collider• fully-polarized, longitudinal and transverse• luminosity: up to few x 1034 e-nucleons cm-2 s-1
Upgradable to higher energies (250 GeV protons)
Pre-booster
Ionsource
Transfer beam line
Medium energy IP
Electron collider ring
(3 to 11 GeV)Injector
12 GeV CEBAF
SRF linacWarm large
booster(up to 20 GeV)
Cold ion collider ring
(up to 100 GeV)
![Page 18: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/18.jpg)
18
solenoid
electron FFQs50 mrad
0 mrad
ion dipole w/ detectors
ions
electrons
IP
ion FFQs
2+3 m 2 m 2 m
Detect particles with angles below 0.5o beyond ion FFQs and in arcs.Need 4 m machine element free region
detectors
Central detector Detect particles with
angles down to 0.5o before ion FFQs.Need 1-2 Tm dipole.
EM
Cal
orim
eter
Had
ron
Cal
orim
eter
Muo
n D
etec
tor
EM
Cal
orim
eter
Solenoid yoke + Muon Detector
TOF
HT
CC
RIC
H
RICH or DIRC/LTCC
Tracking
2m 3m 2m
4-5m
Solenoid yoke + Hadronic Calorimeter
Very-forward detectorLarge dipole bend @ 20 meter from IP (to correct the 50 mr ion horizontal crossing angle) allows for very-small angle detection (<0.3o).Need 20 m machine element free region
MEIC: Full Acceptance Detector
7 meters
Three-stage detection
![Page 19: POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF](https://reader035.vdocuments.net/reader035/viewer/2022062720/56649ef95503460f94c0ae77/html5/thumbnails/19.jpg)
19
My View Going Forward
• There has been excellent progress on developing the EIC science case over the last 2 years, and even more since the INT program.
• There have been important contributions from both the BNL and JLab communities.
• I continue to believe that it is essential that these two communities work together to realize the recommendation of an EIC by the broader nuclear physics community.
• Completing the White Paper is a crucial next step in this process.
• Many thanks to the WP writers/editors.