strings_surf_talk - Caltech High Energy Physics
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Transcript strings_surf_talk - Caltech High Energy Physics
Search for Low Mass Strings at CMS
Andy Yen
Mentor: Harvey Newman
Co-Mentors: Marat Gataullin, Vladimir Litvine
SURF Seminar
October 17, 2009
The Standard Model of Particle Physics
The Standard Model of
particle physics has been
extremely successful in
describing interactions
between elementary particles
There are four known force
carriers and twelve known
quarks and leptons.
However, the model is far
from complete!
There is no theory for
quantum gravity.
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Superstring Theory
There are plenty of reasons to believe in physics beyond
the Standard Model.
One possible alternate model is Superstring theory.
Superstring theory incorporates quantum gravity by
utilizing extra degrees of freedom.
Extension into large extra
dimensions also solves the
hierarchy problem.
Recently demonstrated by
theorists that some superstring
scenarios can be detected at the
LHC.
String mass scale (Ms) < 2 TeV
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The Large Hadron Collider
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The Large Hadron Collider
Luminosity is proportional to the
rate at which collisions occur.
The LHC is scheduled to restart
operation in late 2009.
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The Compact Muon Solenoid
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A New Definition of “Compact”
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Detecting superstrings at LHC
Superstrings can lead to the following non-SM
process: gg→gγ
Extra contribution to the SM photon+jet.
Ms ~ 1 TeV, 100 events for 200pb-1
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Backgrounds
Standard Model photon+jet is the dominant
background.
There is also a significant background from QCD
Dijets
Sometimes, most of the jet energy is in an isolated
neutral meson.
These neutral hadrons decay into a photon pair
which can appear in the ECAL as a single energetic
object.
This can lead to jets being misidentified as
photons.
Misidentified jets can be rejected with high
efficiency, but the cross section is large.
Signal and backgrounds simulated with Monte
Carlo methods.
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Event Selection
Primary objective is to reject QCD
jet fakes.
Cut based selection on a series of
kinematic variables is used.
R9 = S9/S25
H/E = HCAL Energy
ECAL Energy
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Event Reconstruction
Photon reconstruction is close to 98% efficient with
0.5% energy resolution.
Jets are not as well reconstructed
Poor HCAL granularity
Intrinsic fluctuations in hadronic showers
Resolution of reconstructed invariant mass is
dominated by jet resolution.
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Reconstruction Energy Resolution
sisCone algorithm (“seedless infrared safe cone”)
Energy response = Reco Energy/“True” Energy
Peak location: 1.00
Sigma: 0.5%
Peak location: 0.94
Sigma: 8.7%
Photons
Jets
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Collinear Splitting
Even in the sisCone Jet, there is still a tail at low
values.
Approximately 10% of reconstructed Jets have 2nd
Jet within dR<1
Standard sisCone algorithm is optimized for low
energy jets.
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Collinear correction
Take the vector sum of the momentum of the two jets
Use Pt-weighted average of the direction of the two
jets.
Improvements in position and energy reconstruction!
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Invariant Mass Reconstruction
The invariant mass of the
photon+jet can be
calculated from:
2
M e* E p
Luminosity = 100 pb-1
2
Selection efficiency of
68.10% was attained for the
string signal.
Reconstructed mass
resolution of approximately
6% is achieved.
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Estimating Signal Significance
Significance is evaluated based on the number of
observed events compared to the number of expected
background events in the region of the peak.
Random fluctuations in the background can lead to
“accidental” peak-like structures in the spectrum.
Five sigma significance - the probability that a claimed
signal is caused by a local fluctuation of the background
is 2.9·10-7 (very, very improbable!)
A log-likelihood approach is used.
Finally, the significance is given by
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Results
100 pb-1 of integrated luminosity will lead to a discovery
with a significance of 9.84.
A 5 sigma discovery is possible with as little as 25.8 pb-1.
Signal+BG and BG only
distributions for 1000pb-1
of integrated luminosity
and center of mass
energy of 10 TeV.
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Conclusion
These results represent the string theory searches
done at the LHC.
The results show that CMS is capable of making a
discovery during the early running stages.
LHC is currently scheduled to restart in 2 months.
100 pb-1 of integrated luminosity might be possible
within the first year.
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Acknowledgements
Professor Harvey
Newman
Dr. Marat Gataullin and
Vladimir Litvine
Dr. Arunava Roy
Professor Haim Goldberg
Caltech SFP and Rose
Hills Foundation
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The End