Current Research / Experiments
Belle / HERMES / PHENIX / G0 / RCS / nPOL / JLab Transversity
Muon g-2 / MuLan / MuCap / nEDM
Strong Interaction Physics |
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Belle | |
| KEK - Tsukuba, Japan | ||
| Matthias Grosse-Perdekamp, David Hertzog | ||
The Japanese B-factory KEKB in Tsukuba has produced an enormous data sample for e+e- - annihilation into quark-anti quark pairs. We utilize these data to measure subtle spin effects in the fragmentation process of the quarks. The knowledge of spin effects in quark fragmentation is important input to our program to study transverse proton spin structure in the HERMES and PHENIX experiments, and at Jefferson Laboratory. In addition, we carry out analysis in Belle which will lead to improved knowledge of the contribution from hadronic loops to the anomalous magnetic moment of the muon. This analysis is critical input for the interpretation of the
g-2 experiment E821 at Brookhaven National Laboratory. |
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HERMES | |
| DESY - Hamburg, Germany | ||
| Naomi Makins (analysis coordinator) | ||
HERMES is an experiment investigating the quark-gluon
structure of matter: we study the spin structure of the nucleon. By nucleon,
we refer to the protons and neutrons which are the fundamental components of
all atomic nuclei. However, if you look a little closer, you find that these
nucleons are not as fundamental as they might appear... in fact, they are bound
states, composite systems composed of even more fundamental constituents, namely
quarks and gluons, held together by the strong force. And all of these particles
have an important property called spin. The quarks have spin 1/2, the gluons
have spin 1, and the nucleon itself has spin 1/2. The question we seek to answer
at HERMES goes roughly like this: "How do the constituents of the nucleon conspire
to produce its overall spin of 1/2?" Our first data-taking run started in 1995,
and ended in September, 2000. HERMES run 2 started in 2001 and will last up to
summer 2007. [ref] |
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PHENIX | |
| BNL - Long Island, NY | ||
| Jen-Chieh Peng, Matthias Grosse-Perdekamp (deputy spokesperson) | ||
Our understanding of proton
sub-structure is closely connected to the
physics of the quantum chromodynamics (QCD) vacuum at high energy
densities: the properties of the proton cannot be understood without
taking into account the complex "sea" of virtual quark, anti-quark
pairs and gluons inside the proton. In PHENIX, we study the
sub-structure of protons in proton-nucleus and polarized proton-proton
collisions leading to a very broad and rigorous program in the physics
of hadrons and QCD as the theory describing their interactions and
structure. |
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G0 | |
| Jefferson Lab - Newport News, VA | ||
| Doug Beck (spokesperson), Peter Kammel, Steve Williamson (project manager) | ||
The goal of the G0 experiment is to learn more about the quark
substructure of protons and neutrons (nucleons). Our interest is in
the distributions of charge and magnetization in the nucleon and how
it is built up out of the different types of quarks. We are particularly
interested in whether these distributions have any contribution from strange
quarks as this type exists only "virtually" in nucleons as the result
of the quantum mechanical interplay between mass and energy.
[ref] |
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RCS (Real Photon Scattering) | |
| Jefferson Lab - Newport News, VA | ||
| Alan Nathan (co-spokesperson) | ||
The Real Compton Scattering (RCS) experiment measured the cross
sections for RCS from the proton in the energy range 3-6 GeV and over
a wide angular range, and measured the longitudinal and transverse
components of the polarization transfer to the recoil proton at a single
kinematic point. Together, these measurements test models of the reaction
mechanism and determine new structure functions of the proton that are related
to the same nonforward parton densities that determine the elastic electron
scattering form factors and the parton densities.
[ref]
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| nPOL | ||
| MAX-lab - Lund, Sweden | ||
| Alan Nathan | ||
We are attempting to measure the electromagnetic polarizabilities of the neutron by deuteron elastic Compton scattering. By covering a wide range of angles and energies we will reduce the model dependence while still having a smaller statistical uncertainty than previous measurements. Recent theoretical developments in accounting for meson exchange currents inside the deuteron and improvement of the Baldin sum rule should provide us with the ability to accurately determine the electric and magnetic polarizabilities. |
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JLab Transversity | |
| Jefferson Lab - Newport News, VA | ||
| Jen-Chieh Peng (co-spokesperson of E-06-010) | ||
The goal of the JLab Transversity experiment is to provide the
first measurement of the neutron transverse target single spin asymmetry
(SSA) complementary to the recent HERMES and COMPASS measurements on the
proton and deuteron. SSA data on transversely polarized neutrons will
provide crucial new information on the flavor dependence of various
structure and fragmentation functions probed by the SSA experiments.
This first measurement focuses on the valence quark region. Data from
this experiment, when combined with the world proton and deuteron data,
will provide powerful constraints on the transversity distributions and
Sivers function for both u-quark and d-quark in the valence region.
[ref] |
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Fundamental Symmetries |
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Muon g-2 | |
| BNL - Long Island, NY | ||
| Paul Debevec, Dave Hertzog (co-spokesperson), Peter Kammel | ||
The muon anomalous magnetic moment,
measured by the E821 Collaboration
to a precision of 0.54 ppm, represents a stringent test of the Standard
Model. Current (2007) comparison with theory indicates a 3.4 standard
deviation, arguably the strongest experimental hint of new physics apart
from the recent revolution in the neutrino sector. The implications are
profound as the magnitude of the deviation locks squarely with
predictions by many supersymmetric models and implies mass scales that
are quite accessible at the Large Hadron Collider. Toward a more
sensitive experiment, we have strongly pushed the new E969 experiment at
BNL, which aims to reduce the experimental uncertainty by a factor of 2
- 3. The UIUC group has designed a new beamline concept and has built
prototype W/SciFi calorimeters as part of our R & D efforts for E969. |
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MuLan | |
| PSI - Villigen, Switzerland | ||
| Paul Debevec, Dave Hertzog (co-spokesperson), Peter Kammel | ||
The Muon Lifetime Analysis (MuLan) experiment
will measure the positive muon lifetime to a precision of one part per
million (ppm). The muon lifetime provides the most precise determination
of the Fermi coupling constant, which is one of the fundamental inputs to
the Standard Model. Recent advances in theory have reduced the theoretical
uncertainty on the Fermi coupling constant as calculated from the muon
lifetime to a few tenths of a ppm. The remaining uncertainty on the Fermi
constant is entirely experimental, and is dominated by the uncertainty on
the muon lifetime. The MuLan experiment will use an innovative pulsed beam,
a symmetric detector, and modern data-taking methods to reduce the uncertainty
on the muon lifetime to 1 ppm. |
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MuCap | |
| PSI - Villigen, Switzerland | ||
| Dave Hertzog, Peter Kammel (co-spokesperson) | ||
The goal of the µCap experiment is a 1%
precision measurement of the muon capture rate on the proton. From the
capture rate the pseudoscalar form factor gP of the nucleon
will be extracted with 7% precision. This basic quantity is predicted
theoretically with high precision, but the experimental situation is
quite controversial. The new experiment should yield an unambiguous
value for gP and a sensitive test of the chiral symmetry of QCD
at low energies. |
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Neutron Electric Dipole Moment | |
| SNS - Oak Ridge, Tennessee | ||
| Doug Beck, Jen-Chieh Peng, Steve Williamson | ||
The possible existence of a non-zero electric
dipole moment of the neutron is of great fundamental interest and directly
impacts our understanding of the nature of electro-weak and strong interactions.
The experimental search for this moment has the potential to reveal new sources
of T and CP violation and to challenge calcuations that propose extensions to
the Standard Model. In addition, the small value for the neutron EDM continues
to raise the issue of why the strength of the CP-violating terms in the QCD
Lagrangian are so small. This seems to suggest the existence of a new
fundamental symmetry that blocks strong CP-violating processes.
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This material is based upon work supported by the National Science
Foundation under Grant No. NSF PHY 06-01067.
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