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Contributions of Strange Quarks to Proton Structure

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Parity-Violating Electron Scattering. Interference term violates parity: ... Parity-violating elastic electron scattering measures strange quark vector currents ... – PowerPoint PPT presentation

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Title: Contributions of Strange Quarks to Proton Structure


1
Contributions of Strange Quarks to Proton
Structure
Doug Beck UIUC 26 Oct. 2005
  • Outline
  • Physics motivation
  • Experiments
  • Results
  • Speculation

2
Physics Motivation
3
Strange Quark Observables
  • scalar matrix element
  • .
  • see talk by M. Sainio, Th. 245
  • momentum carried by strange quarks
  • .
    NuTEV hep-ex/9906037
  • .
  • spin carried by strange quarks
  • as determined in sum rule
  • Ds -0.1 - 0
  • as determined in semi-inclusive Ds(x)
  • see talk by Hal Jackson (Tues. 230)
  • vector matrix elements (Mon. 230)

CTEQ6M, NLO NuTEV hep-ex/0405037
4
Vector Quark Currents in the Nucleon
  • Measure
  • e.g.
  • note
  • then
  • charge symmetry(see G. A. Miller PRC 57
    (98) 1492.)
  • dropping the p superscripts on the left

5
. , Non-Zero?
  • charge distribution
  • if s, s are separated, non-zero net contribution
  • convection current
  • if s, s are separated, non-zero net contribution
  • spin current
  • spin triplet moments cancel
  • spin singlet zero net moment, zero net
    convection
  • also requires separation

6
Parity-Violating Electron Scattering
  • contributes to electron scattering
  • - interference term large x small
  • Interference term violates parity
    usewhere

7
Experiments
8
Summary of PV Electron Scattering Experiments
publishing, running
publishing, running
2006
published x2, running
published, running
2008
K. Kumar
9
SAMPLE Experiment
Caltech, Illinois, Kentucky, LaTech, Maryland,
MIT, Virginia Tech, WM
  • Measure GM (Q2 0.1 GeV2) for 1H,2H

Z
Ebeam 200 MeV Ibeam 40 mA Pbeam 35 Dq
130 - 170o DW 1.5 sr ltarget 40 cm L
4.3 x 1038 cm-2 s-1 A -7 ppm
10
HAPPEx (JLab Hall A)
  • Measured GEs 0.39 GMs at Q2 0.48 GeV2
  • 2004 runs 1H, 4He at 0.11 GeV2

Ebeam 3.2 GeV Ibeam 50 mA Pbeam 80 q
60 DW (3.7 msr) x 2 ltarget 20 cm L 2 x
1038 cm-2 s-1 A -2, 8 ppm
HAPPEx nucl-ex/0506010
11
PVA4 (Mainz)
  • Measure GEs 0.11 GMs at Q2 0.1 GeV2
  • have also measured at Q2 0.23 GeV2

Second measurement Ebeam 0.57 GeV Ibeam 20
mA Pbeam 80 q 350 DW 0.7 sr ltarget
10 cm L 0.5 x 1038 cm-2 s-1 A -2 ppm
  • Q20.1 GeV2
  • Ameas -1.36 0.29 0.13 ppm
  • Ath -2.06 0.14 ppm
  • PRL 94 (05) 152001

12
G0 Experiment (JLab Hall C)
  • Measure ,
  • different linear combination of u, d and s
    contributions than e.m. form factors
  • strange quark contributions to sea
  • Measure forward and backward asymmetries
  • recoil protons for forward measurement
  • electrons for backward measurements
  • elastic/inelastic for 1H, elastic for 2H
  • Forward measurements complete (101 Coulombs)

Ebeam 3.03 GeV, 0.36 - 0.69 GeV Ibeam 40 mA,
80 mA Pbeam 75, 80 q 52 760, 104 -
1160 DW 0.9 sr, 0.5 sr ltarget 20 cm L 2.1,
4.2 x 1038 cm-2 s-1 A -1 to -50 ppm, -12 to -70
ppm
13
G0 in Hall C (JLab)
superconducting magnet (SMS)
cryogenic supply
beam monitoring girder
scintillation detectors
cryogenic target service module
electron beamline
14
Results
15
G0 Experimental Asymmetries
  • no vector strange asymmetry, ANVS, is A( ,
    0)
  • em form factors Kelly PRC 70 (2004) 068202
  • inside error bars stat, outside stat. pt-pt
    syst.

http//www.npl.uiuc.edu/exp/G0/Forward
D. Armstrong, et al. PRL 95 (2005) 092001
16
Strange Quark Contribution
  • Strange quark contribution to asymmetry

http//www.npl.uiuc.edu/exp/G0/Forward
17
Strange Quark Contribution to Proton
http//www.npl.uiuc.edu/exp/G0/Forward
D. Armstrong, et al. PRL 95 (2005) 092001
18
. , Data _at_ Q2 0.1 GeV2
-0.013 ? 0.028
0.62 ? 0.31
  • Contours
  • 1s, 2s
  • 68.3, 95.5 CL
  • Theories
  • Leinweber, et al. PRL 94 (05) 212001
  • Lyubovitskij, et al.PRC 66 (02) 055204
  • Lewis, et al.PRD 67 (03) 013003
  • Silva, et al.PRD 65 (01) 014016

http//www.npl.uiuc.edu/exp/G0/Forward
19
. , Data _at_ Q2 0.1 GeV2
-0.013 ? 0.028
0.62 ? 0.31
(0.1 GeV2) 2.12
u 2.28 ? 0.21 d 0.03 ? 0.11 s -0.21 ? 0.11
(0.1 GeV2) -1.42
u -0.07 ? 0.11 d -1.14 ? 0.21 s -0.21 ? 0.11
20
Speculation
21
Simple Fits to All Hydrogen Data
  • Fit

with simple forms for ,
à la Kelly
with
from Q2 0.1 GeV2 result, dipole ff
22
Fit to All Hydrogen Data
  • c1 -0.08
  • c2 -0.5
  • d1 -5.7 ? 1.0
  • d2 19 ? 3
  • d3 1
  • LM,S L2 /1.3

2
23
Fit to All Hydrogen Data
  • c1 -0.08
  • c2 -0.5
  • d1 -5.7 ? 1.0
  • d2 19 ? 3
  • d3 1
  • LM,S L2 /1.3

2
Remember the factor of -1/3
24
Future Running Separation of , .
  • HAPPEx (forward angle)
  • reduce uncertainties for H and He by x2-3 at Q2
    0.1 GeV2
  • H at Q2 0.63 GeV2, uncertainties x3 smaller
    than original
  • PVA4 (backward angle)
  • start with H at Q2 0.23 GeV2 is GE lt 0??
  • can run H D for Q2 lt 1 GeV2
  • G0 (backward angle)
  • start with H, D at Q2 0.63 GeV2 cancellation
    of GE and GM at high Q2??
  • scheduled
  • summer 06 H (D) at Q2 0.23 GeV2 is GE lt 0??
  • conditionally approved

s

s
s
25
Summary
  • Parity-violating elastic electron scattering
    measures strange quark vector currents
  • Four new forward angle results in 2005
  • PVA4 H _at_ Q2 0.1 GeV2
  • HAPPEx H _at_ Q2 0.1 GeV2
  • HAPPEx He _at_ Q2 0.1 GeV2
  • G0 H _at_ Q2 0.1 1 GeV2
  • Results self-consistent
  • Emerging picture
  • GM gt 0 at low Q2 - likely
  • some cancellation of GE and GM likely
  • hint that GE lt 0 at medium Q2

s
s
s
s
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