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Neutral Weak Charge Measurements
In the weak interaction, both charged (W+-) and neutral (Z0) bosons may
be exchanged. But while the strength of the weak charged current is related to
Gf, the Fermi coupling constant, the strength of the weak neutral current
is further dependent on a parameter called the weak mixing angle. Precision measurements of the
muon decay rate determine Gf, while precision asymmetry measurements with on-shell Z0
intermediate states largely determine our knowledge of the weak mixing angle.
If the Standard Model of electroweak interactions is complete, then it must
be self-consistent. For example, measurements of the weak mixing angle made
at low energies in atomic parity violation experiments must be consistent with those made at the very high energies
using Z0 particles. We say "consistent" and not "the same" because the couplings of particles
are influenced by virtual particles in the vacuum, and the size
of such perturbations is energy dependent.
The most familiar example of such small pushes and pulls
by ghostly particles occurs in the case of the electromagnetic fine structure constant, alpha.
This coupling is 1/137 at low energies, but is 7% stronger at energies where
the Z0 has been produced.
Lower energies correspond to longer distances, where a particle's charge is more screened
by a cloud of virtual e+e- pairs. With increasing energy, the reaction occurs further
inside this cloud and one sees more of a particle's bare charge.
But while the variation of the coupling with energy for the electromagnetic force is reasonably
well established, for the weak coupling this was only convincingly demonstrated recently
by the SLAC E158 experiment. A low energy program of
measurements will help better determine the weak mixing angle and achieve a better understanding
of theoretical corrections for the extremely heavy virtual particles which modify weak
interactions.
But the most important motivation for such neutral weak-charge measurements is their potential
sensitivity to physics beyond the Standard Model. It is fascinating to realize
that all the particles of nature are present in the vacuum around us, all the
time. Thus, very heavy (TeV-scale) particles which have not yet been observed in
high energy accelerator experiments may reveal themselves by their subtle effects
in precision low energy measurements. In the JLab Qweak experiment we plan to measure the weak mixing
angle in the coupling of an electron to the proton at relatively low energies.
Following that experiment and the JLab upgrade to 12 GeV, we plan to remeasure the
weak mixing angle in an electron-electron scattering experiment called e2ePV.
The JLab Qweak experiment was approved by the JLab Program Advisory Committee with high priority, has
received substantial funding from the US NSF and DOE, the College of William and Mary,
as well as NSERC of Canada, and is currently under construction.
Overview Talks (Qweak and e2ePV Experiments):
Qweak: A Measurement of the Proton's Weak Charge*,
August 2007 DNP Meeting
  PPT
e2ePV Toroidal Conceptual Design*,
December 2006 ElectroWeak Workshop at JLab
  PDF
e2ePV at 12 GeV*,
August 2006 Hall C Workshop
  PPT
e2ePV: Next Step in the Evolution of the Qweak Experiment?,
July 2006 Qweak Collaboration Meeting at JLab
PPT
Outlook for an Improved Moeller Measurement*,
May 2006 PAVI06
PPT
(.PS of Proceedings )
New Physics and 0+ --> 0+,
March 2006 Qweak Collaboration Meeting
PPT
The Weak Charge Program at JLab*,
December 2005 grad student pizza seminar
PPT
Measuring the Proton's Weak Charge,
September 2005 DNP
PPT
Seminar on Qweak(proton)*
PS (1st half)
PS (2nd half)
Technical Talks (fused silica detectors, beam diagnostics, etc.):
Main Detector Status,
July 2008 Qweak Collaboration Meeting
PDF and PPT
All 1st Order Beam Modulation in the 3C Line,
July 2008 Qweak Collaboration Meeting
PPTX
Beam Current Monitor Performance in the June 2008 Beam Test,
July 2008 Qweak Collaboration Meeting
PPTX
Recent WBS1 Activities,
January 2008 Qweak Collaboration Meeting
PDF
Main Detector Status,
July 2007 Qweak Collaboration Meeting
PDF and PPT
Main Detector Status,
April 2007 APS
PPT
Main Detector Status,
January 2007 Qweak Collaboration Meeting
PDF
e2ePV Toroidal Magnet Concept*,
December 2006 Electroweak Workshop at TJNAF
PPT
Toroidal e2ePV Briefly,
July 2006 e2ePV organizational meeting
PPT
Bar QA, Glue prototyping, and Overall Status,
July 2006 Qweak Collaboration Meeting
PPT
Proposed Spot Size Monitor (Qweak Goes Nonlinear),
March 2006 Qweak Collaboration Meeting
PPT
Main Detector Status,
March 2006 Qweak Collaboration Meeting
PPT
Fused Silica Detectors for Hall C*,
January 2006 Hall C Meeting
PPT
Main Detector Status,
October 2005 Qweak Collaboration Meeting
PDF
Voltage Divider Design and Overall Status,
April 2005 Qweak Collaboration Meeting and APS talk
PPT
Detector Beam Test Results,
August 2004 Qweak Collaboration Meeting
PPT
Transmission/Prototype Update,
October 2003 Qweak Collaboration Meeting
PS
Proposed Quartz Bar Tests in the HMS,
May 2003 Qweak Collaboration Meeting
PDF
First Quartz Cerenkov talk,
March 2002 Qweak Collaboration Meeting
PS
PDF
Technical Documents (fused silica detectors, beam diagnostics, experiment requirements, etc.):
If There is Unique Neutral Axis, How Do We Find It?,
June 2008 Technical Note
PDF
Proposed Beam Time Reduction Scenarios for Qweak,
January 2008 draft response to final Jeopardy PAC
PS
Qweak Lightguide Specifications,
June 2006 (Procurement Document)
PS
Microwave Cavity Spot Size Monitor for Qweak,
January 2006 Tech Note
PS
TRIUMF Preamplifier Irradiation Test,
December 2005 Tech Note
PS
How Should We Calculate the Asymmetry for a Single Bar?,
November 2005 Tech Note
PS
Qweak Fused Silica Radiator Specifications,
July 2005 (Procurement Document)
PS
First Look at Test Ticket Data for Qweak D753WKB PMT's,
June 2005 Tech Note
PS
PMT Selection and First Prototype Divider Design,
May 2005 Tech Note
PS
Error Update,
March 2005 Tech Note
PS
A Future JLab Moeller experiment,
December 2004 (internal e2ePV working group report, update of 2002 version)
  PS
Detector Nonlinearity Specification,
September 2004 Tech Note
PS
For further information about our JLab proton experiment (proposal, publications, collaboration, etc.), see
the JLab Qweak(proton) home page