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The quantum field theory framework used to describe
the interactions amongst the known elementary
particles and fundamental forces (the Standard Model
of particle physics) most naturally describes a world
full of particles with zero mass. However physicists
have observed that particles not only have mass, but
their masses differ over many orders of magnitude.
The simplest mechanism to explain particle mass
(called the Higgs mechanism) requires that there be a
new particle, the Higgs boson. Via interactions with
the field associated with the Higgs boson, particles
could acquire mass in a self-consistent manner. The
problem is that despite searching very hard for the
Higgs boson, it remains undiscovered. The theory does
not predict the mass of the Higgs boson itself, so
finding it amounts to a massive hunt for a very
elusive particle.
My research focus is on searches for the Higgs boson,
searches for related particles and precision
measurements needed to help find the Higgs boson or
rule out its existence. I began this work at the
Large Electron-Positron (LEP) collider at the CERN particle
physics facility outside Geneva, Switzerland and I
continue at the Tevatron proton-antiproton collider
at Fermilab,
located near Chicago. These facilities have led the
way as the highest energy particle accelerators in the
world until the recent commissioning of the Large
Hadron Collider (LHC) which now occupies the circular
tunnel that once held the LEP collider. By increasing
the energy available in the particle collisions
created in these accelerators, it becomes easier to
create particles with large masses. This allow the
search for the Higgs to continue into previously
unexplored territory.
I currently spend much of my time working at
the D&empty
experiment, which is a hadron collider detector at
the Fermilab Tevatron. I am currently co-convener of
the D&empty Higgs physics group, which is the group
that performs the data analysis designed to detect the
presence of Higgs bosons should they exist. I am also
co-convener of the Tevatron New Phenomena/Higgs
Working Group. This is the team of Tevatron
researchers who together coordinate the statistical
combination of results from the CDF and D&empty Higgs
searches (amongst other things). Outside my convener
duties, I am heavily involved in searches designed to
find Higgs bosons and in measurements of properties of
electroweak vector bosons (W± and
Z0). I am also interested in the use of
statistical methods in high energy physics and am
active in the HEP statistics community.
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- "Combined Tevatron Upper Limit on gg&rarr H&rarr
W+W- and Constraints on
the Higgs Boson Mass in Fourth-Generation
Fermion Models", D&empty and CDF
Collaborations.
Phys. Rev. D 82, 011102 (2010);
[arXiv.org:1005.3216]
- "Combination of Tevatron searches for the standard
model Higgs boson in the W+W-
decay mode", D&empty and CDF
Collaborations.
Phys. Rev. Lett. 104, 061802
(2010);
[arXiv.org:1001.4162]
- "Search for Higgs boson production in dilepton plus
missing energy final states with 5.4 fb-1
of pp
collisions at &radic s = 1.96 TeV", The D&empty
Collaboration.
Phys. Rev. Lett. 104, 061804
(2010); [arXiv.org:1001.4481]
- "Measurement of trilinear gauge boson couplings
from WW+WZ &rarr l &nu jj events in pp
collisions at &radic s = 1.96 TeV",The D&empty Collaboration.
Phys. Rev. D 80, 053012 (2009);
[arXiv.org:0907.4398].
- "Evidence of WW+WZ production with lepton + jets final
states in ppcollisions at &radic s = 1.96 TeV", The D&empty Collaboration.
Phys. Rev. Lett. 102, 161801
(2009); [arXiv.org:0810.3873].
- "Combined CDF and D&empty Upper Limits on Standard
Model Higgs Boson Production at High Mass (155-200
GeV/c2) with 3 fb-1 of data", The Tevatron
New Phenomena Higgs Working Group [CDF and D&empty
Collaborations].
FERMILAB-PUB-08-270-E(2008);
[arXiv.org:0808.0534].
- "Combined CDF and D&empty Upper Limits on Standard Model
Higgs-Boson Production," The Tevatron New Phenomena Higgs Working
Group [CDF and D&empty Collaborations].
FERMILAB-PUB-09-060-E; [arXiv.org:0903.4001].
- "A combined search for the standard model Higgs
boson at &radic s = 1.96 TeV", The D&empty Collaboration.
Phys. Lett. B 663 26 (2008); [arXiv.org:0712.0598].
- "A search for anomalous heavy-flavor quark production in
association with W bosons",The D&empty Collaboration.
Phys. Rev. Lett. 94 152002 (2005);
[arXiv.org:hep-ex/0411084]; W. Fisher, FERMILAB-THESIS-2005-06(2005).
- "Results of the Tevatron Higgs sensitivity study",
CDF and D&empty Higgs Working Group [CDF and D&empty Collaborations].
FERMILAB-PUB-03-320-E(2003).
- "Search for a Higgs boson decaying to weak boson pairs at
LEP", The L3 Collaboration.
Phys. Lett. B 568 191 (2003); [arXiv.org:hep-ex/0307010].
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