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The Q p weak Experiment: A Search for New TeV Scale Physics via a Measurement of the Proton’s Weak Charge. Measure: Parity-violating asymmetry in e + p elastic scattering at Q 2 ~ 0.03 GeV 2 to ~4% relative accuracy at JLab

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The q p weak experiment

The Qpweak Experiment:

A Search for New TeV Scale Physics via a Measurement of the Proton’s Weak Charge

Measure:Parity-violating asymmetry in

e + p elastic scattering at Q2 ~ 0.03 GeV2

to ~4% relative accuracy at JLab

Extract:Proton’s weak charge Qpweak ~ 1 – 4 sin2W

to get ~0.3% on sin2W at Q2 ~ 0.03 GeV2

tests “running of sin2W”from M2Z to low Q2

sensitive to new TeV scale physics

W.T.H. van Oers


The q p weak experiment

Running coupling constants in QED and QCD

QCD(running of s)

QED (running of )

137 

s

Q2, GeV2

What about the running of sin2W?


The q p weak experiment

+ 

+

“Running of sin2W” in the Electroweak Standard Model

  • Electroweak radiative corrections

  •  sin2W varies with Q

  • All “extracted” values of sin2W must agree with the Standard

  • Model prediction or new physics is indicated.


Le experiments good news bad news

LE Experiments: Good News/Bad News

  • A 1% measurement of a weak-scale quantity, suppressed by an order of magnitude, is sensitive to physics at the scale3 TeV.

  • This is well above present colliders and complementary to LHC.

  • Fine print:

  • Low energy experiments can’t measure Λ or g separately, only Λ /g.

  • With no bump to display, enormous burden of proof on experiment and theory.

  • If limited by systematic errors, a factor of 2 increase in mass scale requires

  • 22 = 4 reduction in the systematic error. (eg, atomic experiments)

  • If limited by statistical errors, a factor of 2 increase in mass scale requires

  • (22 )2 = 16 improvement in statistical figure of merit. (eg, scattering experiments)

  • A factor of 2 increase in Λ /g in the scattering sector may happen only once per generation!

  • Nevertheless, JLab can do that and a bit more.

Courtesy of D.J. Mack


Weak charge phenomenology

Weak Charge Phenomenology

Note how the roles of the proton and neutron are become almost reversed

(ie, neutron weak charge is dominant, proton weak charge is almost zero!)

This accidental suppression of the proton weak charge in the SM makes it more sensitive to new physics (all other things being equal).

Courtesy of D.J. Mack


The q p weak experiment

  • Qpweak is a well-defined experimental observable

  • Qpweak has a definite prediction in the electroweak Standard Model

Qpweak: Extract from Parity-Violating Electron Scattering

As Q2  0

MEM

MNC

measures Qp – proton’s electric charge

measures Qpweak– proton’s weak charge

(at tree level)


The q p weak experiment

Energy Scale of an “Indirect” Search for New Physics

  • Parameterize New Physics contributions in electron-quark Lagrangian

g: coupling constant, : mass scale

  • A 4% QpWeak measurement probes with

  • 95% confidencelevel for new physics

  • at energy scales to:

  • The TeV discovery potential of weak

  • charge measurements will be unmatched

  • until LHC turns on.

  • If LHC uncovers new physics, then precision

  • low Q2 measurements will be needed to

  • determine charges, coupling constants, etc.


The q p weak experiment

Qpweak & Qeweak – Complementary Diagnostics for New Physics

JLab Qweak

SLAC E158

-

(proposed)

Run I + II + III

(preliminary)

±0.006

Erler, Kurylov, Ramsey-Musolf, PRD 68, 016006 (2003)

  • Qweak measurement will provide a stringent stand alone constraint

  • on Lepto-quark based extensions to the SM.

  • Qpweak (semi-leptonic) and E158 (pure leptonic) together make a

  • powerful program to search for and identify new physics.


Model independent constraints

Model-Independent Constraints

Forget about the predictions of any specific new physics model!

Do the up- and down-quarks have their expected SM weak charges?

today

now

-Qw(down)/2

-Qw(down)/2

future

Dot is SM value

-Qw(up)/2

-Qw(up)/2

Constraints by 12C and APV are nearly parallel (N ~ Z). Proton measurement is needed so weak charges can be separated with interesting errors.

Qw(He) where N = Z could provide an important cross-check on Cs APV.

Figures courtesy of Paul Reimer (ANL)


The q p weak experiment

Elastically Scattered Electron

Luminosity

Monitors

Region III

Drift Chambers

Toroidal Magnet

Region II

Drift Chambers

Region I

GEM Detectors

Eight Fused Silica (quartz)

Čerenkov Detectors

Collimator with 8 openings

θ= 8° ± 2°

35cm Liquid Hydrogen Target

Polarized Electron Beam

Overview of the QpWeak Experiment

Experiment Parameters

(integration mode)

Incident beam energy: 1.165 GeV

Beam Current: 180 μA

Beam Polarization: 85%

LH2 target power: 2.5 KW

Central scattering angle: 8.4° ± 3°

Phi Acceptance: 53% of 2p

Average Q²: 0.030 GeV2

Acceptance averaged asymmetry:–0.29 ppm

Integrated Rate (all sectors): 6.4 GHz

Integrated Rate (per detector): 800 MHz


How it works qweak apparatus in geant4

How it Works:Qweak Apparatus in GEANT4

Courtesy of Klaus Grimm (W&M)

Courtesy of D.J. Mack


The q p weak experiment

Anticipated QpWeak Uncertainties

 Aphys/AphysQpweak/Qpweak

Statistical (2200 hours production) 1.8% 2.9%

Systematic:

Hadronic structure uncertainties -- 1.9%

Beam polarimetry 1.0% 1.6%

Absolute Q2 determination 0.5% 1.1%

Backgrounds 0.5% 0.8%

Helicity-correlated Beam Properties 0.5%0.8%

_________________________________________________________

Total 2.2% 4.1%

4% error on QpW corresponds to ~0.3% precision on sin2W at Q2 ~ 0.03 GeV2

(Erler, Kurylov, Ramsey-Musolf, PRD 68, 016006 (2003))

QpW = 0.0716  0.0006 theoretically

0.8% error comes from QCD uncertainties in box graphs, etc.


The q p weak experiment

hadronic:

(31% of asymmetry)

- contains GE,M GZE,M

Constrained by

HAPPEX, G0, MAMI PVA4

axial:

(4% of asymmetry) -

contains GeA,

has large electroweak radiative corrections.

Constrained by

G0 and SAMPLE

Nucleon Structure Contributions to the Asymmetry

Constraints on Ahadronic from other Measurements

Quadrature sum of expected

Ahadronic = 1.5% and Aaxial = 1.2% errors

contribute ~1.9% to error on QpW


The q p weak experiment

The Qweak Apparatus

(Calibration Mode Only - Production & Calibration Modes)

Quartz Cherenkov Bars

(insensitive to

non-relativistic particles)

Region 2: Horizontal drift chamber location

Region 1: GEM

Gas Electron Multiplier

Mini-torus

e- beam

Ebeam = 1.165 GeV

Ibeam = 180 μA

Polarization ~85%

Target = 2.5 KW

Lumi Monitors

QTOR Magnet

Region 3:Vertical

Drift chambers

Collimator System

Trigger Scintillator


The q p weak experiment

QpWeak Toroidal Magnet - QTOR

  • 8 toroidal coils, 4.5m long along beam

  • Resistive, similar to BLAST magnet

  • Pb shielding between coils

  • Coil holders & frame all Al

  • Bdl ~ 0.7 T-m

  • bends elastic electrons ~ 10o

  • current ~ 9500 A

  • Status:  coils wound in France

  •  support stand under

  • construction


The q p weak experiment

Inelastic/Elastic Separation in QpWeak

View Along Beamline of QpWeak Apparatus - Simulated Events

rectangular

quartz bar;

18 cm wide

X 2 meters

long

Central scattering angle: ~8.4° ± 3°

Phi Acceptance: > 50% of 2

Average Q²: 0.030 GeV2

Acceptance averaged asymmetry: –0.29 ppm

Integrated Rate (per detector): ~801 MHz

Inelastic/Elastic ratio: ~0.026%

Very clean elastic separation!


The q p weak experiment

The QpWeak Liquid Hydrogen Target

  • Target Concept:

  • Similar in design to SAMPLE and G0 targets

  •  longitudinal liquid flow

  •  high stream velocity achieved with

    perforated, tapered “windsock”

  • QpWeak Target parameters/requirements:

  • Length = 35 cm

  • Beam current = 180 A

  • Power = 2200 W beam + 300 W heater

  • Raster size ~4 mm x ~4 mm square

  • Flow velocity > 700 cm/s

  • Density fluctuations (at 15 Hz) < 5x10-5

  • Use reversal rate of 270 Hz


The q p weak experiment

Example:

Typical goals for run-averaged beam properties

Position:

Intensity:

keep small with feedback and careful setup

keep small with symmetrical detector setup

Helicity Correlated Beam Properties: False Asymmetry Corrections

DP = P+ – P-

Y = Detector yield

(P = beam parameter

~energy, position, angle, intensity)


The q p weak experiment

Q2Determination

Quartz Cherenkov Bars

(insensitive to

non-relativistic particles)

Region 1: GEM

Gas Electron Multiplier

Region 2: Horizontal drift chamber location

e- beam

Expected Q2 distribution

Region 3:Vertical

Drift chambers

Trigger Scintillator

Use low beam current (~ few nA) to run in “pulse counting” mode with a tracking

system to determine the “light-weighted” Q2 distribution.

Region 1 + 2 chambers --> determine value of Q2

Region 3 chamber --> efficiency map of quartz detectors


The q p weak experiment

Precision Polarimetry

Hall C has existing ~1% precision Moller polarimeter

  • Present limitations:

    • IMax ~ 10 A.

    • At higher currents the Fe target depolarizes.

    • Measurement is destructive

  • Plan to upgrading Møller:

    • Measure Pbeam at 100 A or higher, quasi-continuously

    • Trick: kicker + strip or wire target (early tests look promising – tested up to 40 A so far)

  • Schematic of planned new Hall C Compton polarimeter.


E2epv at 12 gev

e2ePV at 12 GeV

JLab could determine Qw(e) to 2.5% as a search for new physics or the best low energy determination of the weak mixing angle.

  • E = 12 GeV

  • 4000 hours

  • L = 150 cm

  • APV = -40 ppb

Courtesy of D.J. Mack


E2epv at 12 gev1

e2ePV at 12 GeV

Theory contours 95% CL Expt bands 1σ

ΔQw(p)

  • Qw(e) would tightly constrain RPV SUSY (ie tree-level)

  • Killer application of improved Qw(e) is to RPC SUSY

    (ie, loop-level)

    One of few ways to constrain RPC SUSY if it happens to conserve CP (hence SUSY EDM = 0).

    Direct associated- production of a pair of RPC SUSY particles might not be possible even at LHC.

ΔQw(e)

d(QeW)SUSY/ (QeW)SM

Contours courtesy of Shufang Su (U. Arizona)


Future of the jlab weak charge program

Future of the JLab Weak Charge Program

  • Qw(p) finish construction (mid 2007)

    Run I (8%) (2008?)

    (lick wounds following embarrassing confrontation with Mother Nature)

    Run II (4%)

    (Potential 1% Qw(He) as cross-check on Cs APV?)

    What do we do when the LHC (or Atomic Physics) turns our world upside down?

    Will Run II be finished so JLab can respond?

    What do we do if we see a significant deviation in Run II?

2.5% Qw(e) at 12 GeV

Constrain e-e couplings of ~TeV mass particles discovered by LHC.

or

If LHC finds the TeV-scale region is a desert, make world’s best measurement of the weak mixing angle at low energy.

2.5% Qw(p)/Qw(He)

Constrain e-up and e-down quark couplings of ~TeV mass particles discovered by LHC.

Courtesy of D.J. Mack


The q p weak experiment

Summary

  • Completed low energy Standard Model tests are consistent with Standard

  • Model “running of sin2W”

  • SLAC E158 (running verified at ~ 6 level) - leptonic

    • Cs APV (running verified at ~ 4 level) – semi-leptonic, “d-quark dominated”

  • Upcoming QpW Experiment

    • Precision measurement of the proton’s weak charge in the simplest system.

    • Sensitive search for new physics with CL of 95% at the~ 2.3 TeV scale.

    • Fundamental10 measurement of the running of sin2W at low energy.

    • Currently in process of 3 year construction cycle; goal is to have multiple runs in 2008 – 2009 timeframe

  • Possible 12 GeV Parity-Violating Moller Experiment at JLAB

    • Conceptual design indicates reduction of E158 error by ~5 may be possible at 12 GeV JLAB.

    • weak charge triad 

    • (Ramsey-Musolf)


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