dijet resonances kazım z. gümüş and nural akchurin texas tech university
DESCRIPTION
Dijet Resonances Kazım Z. Gümüş and Nural Akchurin Texas Tech University Selda Esen and Robert M. Harris Fermilab PRS JETMET Meeting July 6, 2005. Motivation. We search for narrow resonances decaying to dijets pp g X g Jet Jet (inclusive) - PowerPoint PPT PresentationTRANSCRIPT
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Dijet Resonances
Kazım Z. Gümüş and Nural Akchurin
Texas Tech University
Selda Esen and Robert M. Harris
Fermilab
PRS JETMET Meeting
July 6, 2005
Kazim Gumus, Texas Tech University 2
Motivation
We search for narrow resonances decaying to dijets
pp X Jet Jet (inclusive) We will use Zprime as a first model for dijet resonances, just to get started.
Theoretical motivation:
Lots of new particles decay to dijets. (See next slide)
Experimental motivation:
LHC is a parton parton collider. Resonances made from partons will decay to partons, giving jets.
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Axigluon from Chiral Color: SU(3)L x SU(3)R qq A qq, axial-vector (JP=1+) color-octet particle with half-width /2 .05M
Coloron from extended technicolorqq C qq, vector (JP=1-) color-octet particle with half-width /2 .05M
Excited states of composite quarks qg q*qg, fermion (JP=1/2+) color triplet particle with half-width /2 .02M
Technirhos from Technicolorqq,ggqq,gg, vector (JP=1-) color octet particle with half-width /2 .01M
Diquarks in superstring inspired E6 GUT modelsud D ud, scalar (JP=0+) color triplet particle with half-width /2 .004M
Extra W bosons inspired by left-right symmetric grand unified modelsqq W ’qq, vector (JP=1-) color singlet particle with half-width /2 .01M
Extra Z bosons inspired by grand unified modelsqq Z ’qq, vector (JP=1-) color singlet particle with half-width /2 .01M
Randall Sundrum gravitons in model with large extra dimensionsqq, ggGqq,gg, tensor (JP=2-) color singlet particle with half-width /2 <.05M
Narrow Dijet Resonances(from “New Physics with Dijet” talk given by R.Harris at HCAL/JetMet Workshop, 11/12/2004)
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Cross section
from Robert Harris
Basically, since Zprime is produced with weak force, it has low cross section.
Kazim Gumus, Texas Tech University 5
Data Sample & Software
700 GeV ZprimeData: DC04 data, 400K Zprime decaying to dijets events (Z’ mass 700GeV) We used 50K events.Software: PYTHIA, OSCAR 2_4_5 for sim., ORCA 7_6_0 for digitization. Jet Reconstruction: ORCA_8_4_0. Analysis: JetMetAnalysis/Jets in ORCA_8_4_0. All samples produced with pileup at lum = 2 x 1033 cm-2s-1. RecJetRoot trees were used to write jets on cmsuaf at Fermi lab.
5 TeV ZprimeData: 4526 Zprime decaying to dijets events (Zprime mass 5TeV)Software: CMKIN2_1_0, OSCAR 2_4_6 for sim., ORCA 7_6_0 for digitization. Jet Reconstruction: ORCA_8_7_1. RecJetRoot trees were used to write jets on cmsuaf at Fermi lab. Pileup is not included.
2 TeV ZprimeData: 19500 Zprime decaying to dijets events (Zprime mass 2TeV)Software: CMKIN4_3_1, OSCAR 3_6_5 for sim., ORCA 8_7_3 for digitization. Jet Reconstruction: ORCA_8_7_1. RecJetRoot trees were used to write jets on cmsuaf at Fermi lab. Pileup is not included.
QCD dataSee Selda Esen’s talk given at CMS Physics Week, April 14, 2005
Kazim Gumus, Texas Tech University 6
Jet Reconstruction & Correction
Iterative cone jet algorithm with R=0.5 and E scheme.Generated Jets: particles in the jet cone, excluding pileup.Reconstructed Jets: EcalPlusHcalTowers with ET>500 MeV.Corrected Jets: Reconstructed jets with jetCalibV1 applied.Correction back to particles in jet cone before pileup.
Event Selection
Find the two jets in the event with highest PT: leading jets.Require each leading jet have |eta|<1. Enhances sensitivity to new physics which is produced at low |eta|. Also, Ecal end caps may not be there, or understood, on day 1.Dijet mass: M = sqrt( (E1+E2)2 - (px1+px2
)2 – (py1+py2)2 – (pz1+pz2)2 ).
Cross Section
Bin the dijet mass in ~10% wide bins: bin size increases with mass.Divide rate by the luminosity and bin width: differential cross section
Analysis
(from “New Physics with Dijet” talk given by R.Harris at HCAL/JetMet Workshop, 11/12/2004)
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700 GeV Dijet Mass Distribution
Reconstructed and corrected dijet mass distribution for 700GeV dijets.
Long tail to the low mass is due to final state radiation.
We fit the peak and high mass tail (core) to a gaussian and get mean and .
Kazim Gumus, Texas Tech University 8
2 TeV Dijet Mass Distribution
Reconstructed and corrected dijet mass distribution for 2 TeV dijets.
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5 TeV Dijet Mass Distribution
Reconstructed and corrected dijet mass distribution for 5 TeV dijets.
Rise in the long tail at low mass is due to parton distributions enhancing the tail of the Breit-Wigner resonance at low mass.
Kazim Gumus, Texas Tech University 10
Dijet Resolution (core)
Dijet mass resolution varies from 9.5% at 700 GeV to about 6% at 5 TeV.
Mass bins now roughly 10%, a little larger than resolution. Will reduce them.
Kazim Gumus, Texas Tech University 11
QCD cross section
from Selda Esen
(|eta|<1 )
(Lum=1 fb-1)
There was a bug inthe previously
shown dijet mass cross sections.
They were about a factor of 20 too
small.
This plot is an update, in which the bug has been
removed. The cross section
agrees with a LO QCD calculation.
Kazim Gumus, Texas Tech University 12
700 GeV Dijet Cross section
(|eta|<1, Lum=1fb-1)
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2 TeV Dijet Cross section
(|eta|<1, Lum=1fb-1)
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5 TeV Dijet Cross section
(|eta|<1, Lum=1fb-1)
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Cross section (all)
(|eta|<1 )
(Lum=1fb-1)
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QCD sensitivity
From Selda Esen
600 30 1Trigger Prescales
( Lum = 1 fb-1 )
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Signal sensitivity
(|eta|<1 )
(Lum = 1fb-1)This plot is an update to the one shown in
the SUSY/BSMMeeting on
June 9.
The plot shown on June 9 was affected by the
QCD cross section bug,
and showed too much sensitivity
to a Z’
Kazim Gumus, Texas Tech University 18
Excited quarks are produced with strong interaction. It has significantly higher cross section than Zprime.
We scaled the Zprime events with the ratio of excited quark cross section to the Zprime cross section to see the excited quark sensitivity.
The E6 diquarks have "electromagnetic strength" coupling. However they have competitive cross section compared to excited quarks at high mass, because they are produced from the valence quarks in the proton, which have higher momentum.
Same as excited quarks, we plotted E6 diquark cross section histogram and used it to see its sensitivity.
See next page for results.
Excited quark and E6 diquark
'
*'* )()(
Z
qZq histhist
'' )()(
Z
DZD histhist
Kazim Gumus, Texas Tech University 19
Excited quarks and E6 diquarks
( Lum = 1 fb-1 )
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Conclusions and Future Plans
• Our first look at search for dijet resonances.
• Hard to see a Z’ with 1 fb-1 due to limited statistics for both signal and background: Z’ has a small cross section compared to QCD.– Around 2 TeV, where the unprescaled trigger begins, there is some
sensitivity to a Z’ which may allow observation with larger luminosities (10 – 100 fb-1)
• Sensitivity to excited quarks (strongly produced) and E6 diquarks (produced from valence quarks) are much better than Z’. – We should be able to see these up to a few TeV (3-5) for 1 fb-1. – Our sensitivity to Axigluons or Colorons is similar to excited quarks.
• Working on producing likelihoods to estimate 5 discovery mass reach and 95% CL mass limits for all models (Z’, q*, diquarks, etc.)– Working on the cross section for new models, like technirhos (R. Harris)
• Plan to redo mass binning to correspond to mass resolution.
Kazim Gumus, Texas Tech University 21
Back up Slide
5TeV Zprime (generator particle) mass dist. (CMKIN level)