Weak probe of the nucleon in electron scattering

Download Report

Transcript Weak probe of the nucleon in electron scattering

Weak probe of the nucleon
in electron scattering
•Weak Current far from
the Z pole
•History
•Elastic Scattering and strange
content of the nucleon
•Perspectives in charged
current and DIS kinematics
•Conclusion
David Lhuillier , CEA Saclay
Principle
e’
e’
e
e-
N
e- X
e
g(Q2)
=
N
+
X
Q2 << MZ2 at typical “hadronic scale”
Z0
N
X
Nice perturbative probe
But weak interaction violates P
 Build a pseudo-scalar observable, prop. to MZ:
ALR~GFQ2/4pa
ALR~10-4 at Q2=1 (GeV/c)2
David Lhuillier , CEA Saclay
2
A Bit of History: E122 @ SLAC
DIS off deuteron target:
e’
e
g
2H
•Isoscalar target: fu(x)=fd(x)
•Neglect sea distributions: x > 0.2
David Lhuillier , CEA Saclay
x=Q2/2Mn
y=n/E
,Z0
X
x dependence factorizes out
A bit of History: E122 @ SLAC
First constraint establishing
the Weinberg-Salam Model:
Hybrid
C.Y.Prescot et al,
Phys. Lett. 84B, 524 (1979)
sin2qW=
0.224+/-0.020
Extensions:
•Low x: probe sea contribution with sin2qW as input
•Larger x: precise test of sin2qW
(Jlab LOI, complementary to E158 and Qweak)
David Lhuillier , CEA Saclay
Factor 1000 !
Parity Violation in e- Scattering
Test SM
Elastic
e--N
Mutual enrichment between test of SM and hadronic structure
Impressive performances of polarized beam
David Lhuillier , CEA Saclay
Experimental Techniques
Key elements:
Injector
Source
•High Pe and I
•Rapid helicity flip
•Feedbacks
Beam line
Hall
l/2
“Table-Top” Experiments
Half-wave plate reversals
IN
OUT
Charge asymmetry
at 1 GeV
Final: AI=-8.4+/-7.8 ppb (10-9) !
David Lhuillier , CEA Saclay
Elastic Scattering
e’
e’
e
e-
e- N
N
2
e
g(Q2)
=
N
+
N
Z0
N
N
Electromagnetic FF
Weak FF
ALR=
GFQ2
2pa 2
David Lhuillier , CEA Saclay
f(F1g,F2g,F1Z,F2Z,GA)
few ppm
at Q2<1 (GeV/c)2
Strange content of the Nucleon
Sum over 3 quarks flavours (u,d,s)
weighted by elec. and weak charges
Charge symmetry
Extraction of the strange quarks contribution
3x3 equations
Same relations
stand for GE/GM…
Motivation triggered by DIS results on Ds but the measured matrix elements
are independent: vector <N|sgms|N> instead of pseudo-vector <N|sgmg5s|N>
David Lhuillier , CEA Saclay
Leading Non Zero Moments
Measurements at low Q2
Scale: <r2n>Sachs=0.12 fm2
Strange Magnetic Moment:
Scale: mN
David Lhuillier , CEA Saclay
<rs2>Sachs (fm2)
Strange Charge Radius:
Elastic e-p Asymmetry
ms= -0.3
<rs2>Sachs= 0.33 fm2
Forward angle:
GsE,GsM
Backward angle:
GsM,GA
David Lhuillier , CEA Saclay
Experimental Strategy
Complete Separation GE/GM/GA
over Q2=0.11 (GeV/c)2
Rosenbluth Method
Forward and backward measurements with the same detector setup
G0 @ Jlab
Q2=0.3-0.8 (Gev/c)2
PVA4 @ MAMI
Q2=0.1 and 0.25 (Gev/c)2
but not enough lever arm to extract the 3 contributions
David Lhuillier , CEA Saclay
Experimental Strategy
Complete Separation GE/GM/GA
over Q2=0.11 (GeV/c)2
Quasi-elastic e-Deuteron
Different targets
Elastic e-4He:
SAMPLE
MIT-Bates
HAPPEx2
JLab
Q2=0.1 GeV/c2
David Lhuillier , CEA Saclay
Isoscalaire Transition pure GE
Experimental Program
Q2 dependence
G0, PVA4, HAPPEx1
0.2 < Q2 < 0.8 (GeV/c)2
First moments
SAMPLE, HAPPEx2, PVA4
Q2 = 0.1 (GeV/c)2
•First Constraint on ms:
ms=0.37+/-0.20stat+/-0.26syst+/-0.15theo
•Expected combined accuracy:
dms ~ 0.16 mN
David Lhuillier , CEA Saclay
d<rs2>Sachs ~ 0.020 fm2 ~ <rn2>Sachs/6
Weak Charged Current
in e-p scattering
0
W- Z W+
The NEPTUNE experiment
n
e-
Letter Of Intent at JLab (A. Deur)
W-
p
n
V
GE,M GA GP
David Lhuillier , CEA Saclay
+
•High luminosity
•Direct measurement
-
•Only detected particle = n
NEPTUNE Experimental Setup
•Background reduction:
Backward kinematic
Sweepnig magnet
Recoil detector
Pulsed beam
e-
S/B~0.1
•APV=10%
Symmetric w.r.t. beam axis
(not represented)
David Lhuillier , CEA Saclay
Accurate
normalization
despite bad S/B.
NEPTUNE Projected Results
n
e-pnn
p electroproduction
GA
E=1-2 GeV
qe=120deg
Q2=0.8-2.7
Q2
(GeV/c)2
Accurate data in an unexplored kinematical domain
of a fundamental observable of the nucleon
David Lhuillier , CEA Saclay
Parity Violating Asymmetry in e-p DIS
e’
e+,e-
g ,Z0
p
Extract G3  separate valence and sea contributions …
David Lhuillier , CEA Saclay
X
Parity Violating Asymmetry in e-p DIS
Single spin asymmetry:
•G3 term is suppressed
•but ratio G2/F2 depends on d/u
•ALR ~ 10-5 Q2, allows accurate
measurements
Charge asymmetry:
[se+-se-] a xG3
David Lhuillier , CEA Saclay
•First data from HERA,
Stat. Limited
•Intense neutrino beams
Conclusion
Weak Neutral Current in e- scattering:
•New probe of the nucleon structure
•Important experimental program ongoing to extract
the contribution of strange quarks to the vector
matrix element <N|sgms|N>.
Development of experimental techniques
•Perspectives in charged current (GA)
and DIS neutral current (d/u).
•Precise test of the interaction itself
David Lhuillier , CEA Saclay
Back to the Future
•New results from ALR in Moller scattering from E158 at SLAC.
•Parity violating asymmetries allow precise test of SM at low energy
David Lhuillier , CEA Saclay