Indiana University High Energy Physics
and Astrophysics Seminars
2003-2004 Academic Year
| Mondays, 4pm | Refreshments 3:30 pm |
| Swain West 238 | HEP Coffee Room (SW262) |
Organizers: Mike Berger and Mark Messier
Fall Semester 2003
| Sep. 1: | NO SEMINAR THIS WEEK |
| Labor Day | |
| Sep. 8: | Degenerate Fermions in Slightly More than One Dimension |
| Brett Altschul | |
| Indiana U.
In one spatial dimenion, a system of low-temperature fermions displays many
remarkable properties. The coherent fermion-hole excitations of the system
behave like bosons, with a spectrum that remains exactly solvable even in the
presence of certain arbitrarily strong interactions. This phenomenon is
described by the Luttinger and Tomonaga-Luttinger models. I shall review
these models and then move on to consider the corrections to their results
that arise when the one-dimensional system is embedded in the real
three-dimensional universe. These corrections, which can be obtained in
several complementary ways, have obvious applications to the future study
of low-temperature fermion trapping.
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| Sep. 15: | The New Ds States: the view from CLEO |
| Jon Urheim | |
| Indiana U.
This past April, the BaBar Collaboration announced the surprising
discovery of a new narrow resonance decaying to Ds+ pi0. Within
a month, confirmation of this state as well as evidence for the
existence of a second narrow Ds state were reported by CLEO.
Confirmation and further elucidation of the properties of both
states came from the Belle Collaboration shortly thereafter.
I will summarize the experimental developments, present the
evidence for the two states, and talk about why the new states
were not expected (but perhaps should have been).
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| Sep. 22: | Revisiting Yukawa Unification |
| Kazuhiro Tobe | |
| University of Michigan
Minimal SO(10) Supersymmetric Grand Unified Theory (SUSY GUT)
is one of interesting candidates for physics beyond the standard model:
all quarks and leptons (including right-handed neutrino) in one generation
are unified into 16-dimensional representation of SO(10), and two Higgs
doublets in SUSY standard model are also unified in 10-dimensional
representation. In this talk, third family Yukawa unification, as
predicted by minimal SO(10) SUSY GUTs, is revisited.
Since GUT-scale Yukawa couplings are very sensitive to SUSY threshold
corrections at weak scale, Yukawa unification hypothesis strongly
constrains low-energy SUSY particle spectrum.
I show constraints on the SUSY spectrum required for Yukawa
unification. I also show that there is an interesting
SUSY parameter region in which the unified Yukawa coupling is unified
into the unified gauge coupling (Gauge-Yukawa unification).
Gauge-Yukawa unification can be realized in higher dimensional models.
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| Sep. 29: | The MIPP Hadron Production Experiment (E907) |
| Nick Graf | |
| Indiana U.
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| Oct. 6: | Recent Results from D0 - Part 1 |
| Daniela Bauer | |
| Indiana U.
The upgraded D0 detector at the Tevatron proton-antiproton collider at Fermilab has been taking data since April 2001. Since then 214 pb-1 of data have been recorded and the first physics results are beginning to emerge.
At a center-of-mass energy of 1.96 TeV the Tevatron provides an excellent opportunity to study heavy quarks. In this talk I will review on-going analyses concerning the beauty and top quarks. This includes cross-section and lifetime measurements and rare decays for B-mesons
and cross-section and mass measurements for the top-quark.
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| Oct. 13: | Recent Results from D0 - Part 2 |
| Kyle Stevenson | |
| Indiana U.
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| Oct. 20: | Measurement of W mass and width at LEP 2 |
| Ambreesh Gupta | |
| University of Chicago
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| Oct. 27: | The EXO Neutrinoless Double Beta Decay Experiment |
| Carter Hall | |
| Stanford University
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| Nov. 3: | Cracking the CKM Triangle - BABAR's Next Step |
| Masahiro Morii | |
| Harvard University
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| Nov. 10: | |
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| Nov. 17: | The Physics and Technology of BTeV |
| Rob Kutschke | |
| Fermilab
The BTeV experiment is designed to challenge the Standard Model
explanation of CP violation, mixing and rare decays of hadrons
containing beauty or charmed quarks, an important component
in the broader study of flavor physics. The experimental
apparatus will be a forward spectrometer located at the C0 collision
region of the Tevatron proton-antiproton collider at Fermilab.
The experiment is still being developed; installation is scheduled to start in
2006, followed by commissioning in 2008, and data-taking in 2009.
This seminar will survey the physics goals of the experiment and
describe how these challenges will be met by the chosen design.
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| Nov. 24: | NO SEMINAR THIS WEEK |
| Thanksgiving Week | |
| Dec. 1: | Muon g-2 Experiment at Brookhaven |
| Jonathan Paley | |
| Boston University
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| Dec. 3:
Wednesday 10am SW251 |
Quarkonium production at D0 |
| Jundong Huang | |
| Indiana U.
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| Dec. 8: | On Lorentz-violating Electrodynamics |
| Quentin Bailey | |
| Indiana U.
Lorentz violation is a promising probe for low-energy signals from Planck-scale physics. The Standard-Model Extension (SME) is a general theoretical framework describing effects of Lorentz and CPT violation. In this talk, I will focus on some Lorentz- violating effects arising in the photon sector of the SME. An experiment based on these effects could substantially improve the attainable sensitivity to certain types of Lorentz violation.
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| Dec. 10:
Wednesday 11am SW251 |
Measurements of the Electromagnetic Sachs Form Factors of the Proton in the Time-like Region at Fermilab |
| Seon-Hee Seon | |
| University of Minnesota
E835 was a fixed target pbarp annihilation experiment at Fermilab, which was tuned at 3 GeV < E_cm < 4GeV. Here I describe the measurements on the electromagnetic structures of the proton via an exclusive process pbarp-->e+e-. We measured magnetic Sachs form factor
(G_M) of the proton at s = 11.63, 12.43 and 14.40 GeV^2 via the cross section measurement of the process. The ratio of the two Sachs form factors (G_E/G_M) was measured at s = 13.56 GeV^2 via the angular distribution measurement of the process. The form factor study in E835 provides a good counterpart of the same measurements in the space-like region.
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