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Randall- Sundrum Gravitons and Black Holes at the LHC. Kevin Black Harvard University For the ATLAS and CMS Collaborations. Outline. TeV Scale Gravity Gravitons Black Holes Summary. Landsberg. State of the Standard Model. Effective model which describes data well - PowerPoint PPT Presentation
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Randall- Sundrum Gravitons and Black Holes
at the LHC
Kevin Black
Harvard University
For the ATLAS and CMS Collaborations
Outline
TeV Scale Gravity Gravitons Black Holes Summary
Landsberg
State of the Standard Model
Effective model which describes data well
Accommodates but does not explain Fermion masses CP-Violation
Well known fine-tuning, hierarchy, triviality problems
LEP EWWG – Winter 2007
mH2 ~ ~
MPl2
Why Gravity at the LHC View Standard Model as
effective theory as a low energy approximation
New theory takes over at energy scale comparable to the Higgs mass 1 TeV SUSY, Technicolor, Little
Higgs, .. Perhaps there is no other
scale , GUT scale is ~ TeV Gravity made strong by extra
dimensions where gravity propagates
Randall – Sundrum Model SM fields on one of two
4-dimensional brane in a 5-D space time
Graviton can propagate in the bulk
Kaluza-Klein States on the order of TeV
Main parameters: Mass of Graviton Curvature parameter
( c = k/Mpl) Signatures in dilepton,
diboson, dijet final states
wk = MPl e-kr
q
q
l
l
Current Direct Limits
CDF Conference note 9160 PRL 100, 091802 (2008)
Mass limits from 300 – 900 GeV depending on coupling
Dimuon Signature Two reconstructed muons
One || < 2.1 One with PT > 24 GeV
Use angular distribution to discriminate spin
Main background SM Drell-Yan
c = 0.01c = 0.02c = 0.05c = 0.10
10 fb-1
100 fb-1
300 fb-1
See Dilepton Talk Later this session
Diphotons
Branching ratio twice as large as dilepton
Z’ doesn’t decay into diphotons Backgrounds
Direct Diphoton Production Photon + Jet Dijets (photon misidentification) Drell-Yan (missing tracks)
Two isolated photons with ET > 150 GeV Isolated both by calorimeter and
tracker
Dijets
Two jets | Fit invariant mass (leading 2 jets) Compare observed/predicted Including Systematics
Jet Energy Scale Jet Resolution Trigger Prescales Radiation
See Dijets talk later this session…
Black Holes
Dimopolous, Landsberg Black holes could form if
two colliding partons have impact parameter smaller than RS
Partonic Cross-Section given by geometry, total cross-section convoluted with PDFS
Decay by Hawking Radiation Demographic Decay Spherically Symmetric
E/2
E/2b
b < Rs(E) BH forms
RS2
Black Holes – Generator Studies
CATFISH Collider
grAviTational FIeld Simulator for black Holes
Comput.Phys.Commun.177:506-517,2007
Black Hole – CMS I Parameters
Plank Scale 2 TeV Black Holes 4 – 10 TeV
Signature high sphericity high ΣpT high multiplicity
Backgrounds tt, W/Z + jets, Diboson,
multijets Selection
MBH(reco) > 2 TeV Multiplicity > 4 Sphericity < 0.28
Black Hole – CMS II
ATLAS Black Holes Event Selection
Electron or muon with ||pT > 50 GeV Two approaches (almost identical results)
|pT| > 2.5 TeV (jets + leptons) At least 4 jets and lepton pT > 200 GeV
A n=2,m = 5-14 TeV
C n=2,m = 8-14 TeV
B n=4,m = 5-14 TeV
D n=7,m = 8-14 TeV
ABCD
ATLAS Black Holes 2
Reconstruct the visible mass of the black hole from all objects and MET
Very dramatic signature + large signal cross-sections
ATLAS Black Holes 3
Investigated Event Shapes Do give separation with
background Very different for different
parameters
ATLAS Black Holes 4
Discovery potential S/B > 5 S > 10
Discovery possible ranging from Few pb for 5 TeV ~1 fb for 9 TeV
Summary
Signatures from Gravitons and Black Holes would be dramatic compelling signatures
RS Gravitons should be observable ~5 TeV range and quickly observable for ~1 TeV masses
Black holes could be seen to very high masses (8-9 TeV) with a few to ~ 30 fb-1 of data (depending on parameters)
For older results go to ATLAS and CMS exotics pages
New ATLAS results expected to be made public ~few months…
Backup
Graviton Signatures at the LHC
Gravitons couple to momentum tensor (contribute to most SM processes)
Monojets Single Vector Boson
production Dilepton/Dijet/Diboson
production As resonance As non-resonant
modification to SM cross-section
q
q
g
g
g
G
g
G
q
q G
V q
q G
V
q
q
l
l
q
q
V
V
Backup Dimuon I
Signal Cross-Sections
Drell-Yan Backgrounds – others on ~ 10 to 40 times smaller
Dimuon Backup II
Dimuon Backup III
Dimuon backup 4
Systematics Theory QCD and EW Scale – 13-17% PDF – 7%
Systematics Experiment Misalignment Pileup - negligible Background Shape – 10-15% shift in signficance Trigger –negligible (normalizations float in fit) Magnetic Field – negligable
Dimuon Backup 5
C = 0.01
C= 0.1
Solid line – idealDotted – long term alignmentDashed – “first alignment”
Diphoton Backup IDiphoton production
Photon + Jet
Dijet
Drell-Yan
Diphoton Backup II
Diphoton Backup III
Diphoton Backup 4Hard Process Scale PDF Uncertainties
Dijet Backup
Sezen Sekmen SUSY 07
Sezen Sekmen SUSY 07
CMS Black Hole Backup
Sphericity
PDF Uncertainties :
Uncertainty on Signficance ~ 12%
Black Hole Backup
CMS TDR -2006
Atlas Black Hole backup
As a function of black hole threshold