|
|
John
Negele, Stefano Capitani, Patrick Dreher, Alvaro
Montero, Andrew Pochinsky, Dru Renner, James Steele,
and Uwe-Jens Wiese, Massachusetts Institute of Technology
Robert Edwards, Thomas Jefferson National Accelerator
Facility
Thomas Lippert, Hartmut Neff, and Klaus Schilling,
Universität Wuppertal
 |
|
|
|
Topological
excitations of the gluon field in QCD, which play an important role
in generating quark masses and interactions, can be identified by
localized quark zero modes. The gluon topological charge (left)
and corresponding quark zero mode (right) are shown for a meron
pair on a lattice in an ongoing project to explore the role of these
configurations in producing quark confinement
|
|
Research
Objectives
The major focus of the work is on two key issues: Understanding the role
of instantons and their associated quark zero modes in nucleon structure,
and using the quark zero modes to calculate the sea quark content of the
nucleon. This project has several physics objectives. By calculating the
spectrum for an ensemble of configurations, we expect to understand the
spectrum and the degree of separation of physical modes from unphysical
doublers, and to check the relation between the density of fermion modes
with low virtuality and the chiral condensate. We will carry out a high
statistics study of the degree to which hadron propagators are dominated
by zero modes. We will reconstruct the topological charge density from
the quark eigenmodes to obtain an unambiguous determination of the instanton
content of the QCD vacuum. We will use the zero modes to calculate the
disconnected diagrams corresponding to the strange quark content of the
nucleon.
Computational
Approach
We calculate the low eigenmodes of the Dirac operator using the k-step
Arnoldi method. This method has compelling advantages for our work. First,
since it works in a fixed dimension space, there is no degradation of
orthogonality and corresponding loss or duplication of modes. Second,
its insensitivity to the quark mass makes it extremely useful near the
chiral limit of low pion mass. We have two complementary implementations.
One is an exploratory code in which we can control the region of eigenvalues
at will. The other uses the robust and well-optimized PARPACK package
from ORNL.
Accomplishments
We began major production late in the fiscal year, but we have verified
that our truncated eigenvector approach provides a statistically superior
signal to that obtained with conventional stochastic estimators. Results
show that using 300 low-lying eigenmodes significantly increases the signal.
Significance
This project will develop a new method that can attain a higher level
of statistical accuracy than existing methods and will provide the essential
quark zero modes necessary for these calculations. In addition to elucidating
the physics for timely parity-violating electron-scattering experiments,
this new method should also enable the evaluation of the disconnected
diagrams encountered in deep inelastic electron scattering.
We
will perform the first quantitative study of the eigenmodes for a full
ensemble of configurations. This will enable us to perform the most precise
explorations to date of the eigenvalue spectrum of the Dirac operator,
the separation of physical modes from lattice artifacts, the instanton
content of the QCD vacuum, the quantitative accuracy of the 't Hooft interaction,
and the relation between the density of eigenvalues and the chiral condensate,
as expected from the Banks-Casher formula.
Publications
James V. Steele and J. W. Negele, "Meron pairs and fermion zero modes,"
Phys. Rev. Lett. (in press); hep-lat/0007006.
John
W. Negele, "Instantons, the QCD vacuum, and hadronic physics," Nucl. Phys.
B (Proc. Suppl.) 73, 92 (1999); hep-lat/9810053.
O.
Jahn, F. Lenz, J. W. Negele, and M. Thies, "Center vortices, instantons,
and confinement," Nucl. Phys. B (Proc. Suppl.) 83, 524 (2000).
http://www-ctp.mit.edu/~negele/
|