New Physics with Jets in the Final State at CMS

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Presentation transcript:

New Physics with Jets in the Final State at CMS Paolo Rumerio, Univ. of Alabama On Behalf of the CMS Collaboration Physics at the LHC Vancouver, June 8, 2012 1

Introduction Several BSM searches based on or involving jets and MET have been performed with the 2011 dataset at CMS See Arnd Meyer's talk for lepton-based searches All analyses use the latest techniques refined with the 2011 dataset (dedicated talk by Keti Kaadze on jets and MET). Shown here: Highly boosted all-hadronic tt (5 fb-1) RS Graviton and W' in di-bosons (3 analyses, 4.7 – 5.0 fb-1) Black Holes (4.7 fb-1) Dark Matter and Large Extra Dimensions (4.7 fb-1) Search for three-jet resonances (4.7 fb-1) Di-jet resonances (pair produced or using di-jet angular ratio, 2.2 fb-1) Full list: https://twiki.cern.ch/twiki/bin/view/CMSPublic/PhysicsResultsEXO While the remaining 2011 searches are being finalized/reviewed, the analysis of the 2012 dataset is fully ongoing Paolo Rumerio, University of Alabama June 8, 2012 2

The CMS Detector Paolo Rumerio, University of Alabama June 8, 2012 3

tt Production in Highly Boosted All-Hadronic Final States (EXO-11-006) arXiv:1204.2488 Paolo Rumerio, University of Alabama June 8, 2012 4

Boosted tt New physics scenarios often involve enhanced tt production at high inv. mass Topcolor Z' and Kaluza-Klein Gluon Models propose enhanced tt cross section to resolve the anomalous forward-backward asymmetry measured at the Tevatron 46% of tt production decays into 3+3 jets Due to t and t boost, decay products merge Look at jet substructure to recover this phase space Jet reconstruction: Cambridge-Aachen algorithm with R=0.8 – last algo steps reversed to study sub-jet characteristics Paolo Rumerio, University of Alabama June 8, 2012 5

Boosted tt Type 1: fully merged jet with 3 sub-jets Type 2: two jets, one with 2 sub-jets Top-tag (140<mjet<250 GeV) applied to Type 1 and Type 2 W-tag (60<mjet<100 GeV and cut on 'mass-drop') applied to the jet with 2 sub-jets in Type 2 Type 1 + Type 1 Type 1 + Type 2 Jet mass (MC) Top tag The simulated jet mass for NTMJ MC (light yellow histogram) and Z′ MC (open histogram). Probability to mis-identify a non-top QCD jet with the top tagging algorithm. This is measured from the data and applied to an appropriate "pretag" selection to estimate the QCD background. (data) Paolo Rumerio, University of Alabama June 8, 2012 6

Boosted tt Type 2 candidates: W-jet mass (top-left) W+b mass (top-right) Mass drop variable (bottom-right), used in the W-jet tagging and defined as the mass of the highest mass sub- jet divided by the mass of the jet Exo11006 LEFT PLOT: W mass measurement from within jets using the jet pruning algorithm. This is a boosted muon-plus-jets sample, and what is plotted is the mass of the highest mass jet in the hemisphere away from the muon. From this plot we can extract the subjet jet energy scale comparison between data and MC, which is measured to be 1.01 +- 0.01 (statistical error only). This plot can also be used to measure the efficiency of the W mass cut in the data and the Monte Carlo, which can be used to extract the data-to-MC scale factor. Combining the efficiency scale factor of the "mu" cut (see below), the data-to-MC scale factor of the W tagging algorithm is 0.97 ± 0.03. Paolo Rumerio, University of Alabama June 8, 2012 7

Boosted tt XXX tt mass distributions Exo11006 Observed and predicted ttbar invariant mass distribution in the "1+1" and 1+2 analysis. The continuum ttbar background is taken from the MC prediction. The QCD background is taken from a "mass-modified-mistag" data-driven estimate. Paolo Rumerio, University of Alabama June 8, 2012 8

Boosted tt Likelihood fit to tt mass distribution 95% CL limit on σ x B.R. Extracted using CLs method Exo11006 Topcolor Z' excluded between masses of: 1.3-1.5 TeV for 1% width 1.0-1.6 TeV for 3% width 1.0-2.0 TeV for 10% width Randall-Sundrum Kaluza-Klein gluon excluded in 1.4-1.5 TeV and small region close to 1 TeV Counting technique poses a <2.6 limit on possible cross section enhancement w.r.t SM expectation for tt mass > 1 TeV (a priori most probable value is 2.5) Limits on the possible cross section times branching ratio of ttbar resonances. This plot uses Z' sample with 1% width assumption. Limits on the possible cross section times branching ratio of ttbar resonances. This plot uses Randall-Sundrum Kaluza-Klein gluon samples. Paolo Rumerio, University of Alabama June 8, 2012 9

Search for Randall-Sundrum Gravitons G* → ZZ → qqvv (EXO-11-061) G*/W' → VZ → qqll (EXO-11-081) G* → ZZ → qqll (EXO-11-102) Paolo Rumerio, University of Alabama June 8, 2012 10

RS Graviton Warped Extra Dimension to solve hierarchy problem Leads to a Kaluza-Klein tower of states, k/MPl = coupling parameter To be detected as massive, universally coupled, spin-2 resonances G* → ZZ → qqνν (with qq merged in a single jet) G*/W' → VZ → qqll (with qq merged in a single jet) G* → ZZ → qqll (uses angular spin correlations to discriminate S and B) Paolo Rumerio, University of Alabama June 8, 2012 11

RS G* → ZZ → jet+MET Jet algo: anti-kT with cone size R=0.7 Main selection: jet pT and MET >300 GeV; mjet>70 GeV; MT(jet,MET)>900 GeV; no more than 2 jets pT>30 GeV (2-jet evts kept if Δφ<2.8); no isolated leptons. Bkg determined from data side bands in mjetvs MT(jet,MET) ('ABCD' method) SM background estimate = 153±29 events; observed in data = 138 events Paolo Rumerio, University of Alabama June 8, 2012 12

RS G* → ZZ → jet+MET Likelihood fit performed on signal and side bands regions of mjetvs MT(jet,MET) Upper limit on σ x BR set using CLs method RS Graviton excluded in mass range of 1.0-1.5 TeV for k/MPl above [0.11, 0.29] Paolo Rumerio, University of Alabama June 8, 2012 13

G*/W' → VZ → qqll Heavy Resonance assumption: boosted decay products qq merged into a single jet → 65 < mjet< 120 GeV Leptons (ee or μμ) with small opening angle → care in applying isolation Dominant bkg is Z+jets, then tt → determined from data in side band 30 < mjet< 65 GeV W'SSM excluded between 700 and 929 GeV RS Graviton excluded between 700 and 924 for k/MPl = 0.05 These results are not as competitive as the ones derived in the gammagamma and ll channel searches (mRS > 1500 GeV). However, one should consider that those are derived assuming a democratic RS model. In more recent studies, RS models with SM fields propagating have been proposed, in which case the RS graviton does not couple to fermions. This opens the possibility to an enhancement of the branching ratios for final states with V pairs, as well as the interest to study large values of k/MPl [35]. In this scenario, the current results provide important constraints that are complementary to the ones from the search of resonances decaying to boosted top pairs [36]. The results derived in this analysis are currently the most stringent in the V pair channel. Paolo Rumerio, University of Alabama June 8, 2012 14

RS G* → ZZ → qqll Explores the MZZ region between 400 and 1000 GeV Uses angular likelihood discriminant to suppress bkg Events categorized according to 0, 1, 2 b-tagged jets Di-jet and di-lepton masses consistent with Z Jet kinematics corrected by fitting imposing mjj=mZ Excluded Gravitons with mass M1 < 945 GeV for k=0.1, and M1 < 720 GeV and 760 < M1 < 850 GeV for k=0.05 These results are not as competitive as the ones derived in the gammagamma and ll channel searches (mRS > 1500 GeV). However, one should consider that those are derived assuming a democratic RS model. In more recent studies, RS models with SM fields propagating have been proposed, in which case the RS graviton does not couple to fermions. This opens the possibility to an enhancement of the branching ratios for final states with V pairs, as well as the interest to study large values of k/MPl [35]. In this scenario, the current results provide important constraints that are complementary to the ones from the search of resonances decaying to boosted top pairs [36]. The results derived in this analysis are currently the most stringent in the V pair channel. Paolo Rumerio, University of Alabama June 8, 2012 15

Search for Microscopic Black Holes (EXO-11-071) 10.1007/JHEP04(2012)061 Paolo Rumerio, University of Alabama June 8, 2012 16

Black Holes ADD model proposed to solve the hierarchy problem: By introducing n large, flat, extra spatial dimensions Scale for new physics given in terms of multi-dim Planck scale MD One prediction is the formation of microscopic Black Holes Spectacular signature with large number (N) of energetic particles (75% jets, 25% W/Z/γ/leptons) Selection requires ST = ∑ pT of jets, γ's, l's + MET above a 50 GeV threshold Dominant background at high ST is QCD multijet production Determined from data exploiting the empirically observed ST multiplicity invariance Paolo Rumerio, University of Alabama June 8, 2012 17

Black Holes Total transverse energy (ST) distribution for multiplicity N ≥ 4 events, and expected semiclassical BH signals Model-independent 95% CL limits (CLs method) on N ≥ 4 cross section for ST > STmin versus STmin (limits provided for N ≥ 3,4,5,6,7,8) new Paolo Rumerio, University of Alabama June 8, 2012 18

Black Holes Limits are set on specific subsets of the probed models using optimized ST and N selections. For example: Minimum Quantum BH mass excluded at 95% CL vs. reduced Planck scale MD for n=1 (RS model) and n=2-6 (ADD model) Minimum BH mass excluded at 95% CL vs. reduced Planck scale MD for n=2,4,6 Paolo Rumerio, University of Alabama June 8, 2012 19

Large Extra Dimensions in Monojet Events Dark Matter and Large Extra Dimensions in Monojet Events (EXO-11-059) Paolo Rumerio, University of Alabama June 8, 2012 20

DM and LED A monojet + MET signature arises in Large Extra Dimenstions (LED) of ADD model → G escapes in extra dim. space Dark Matter interaction with SM mediated by very heavy particles Selection: jet (anti-kT R=0.5) pT > 110 GeV; MET > 350 GeV; ≤2 jets pT>30 GeV (2-jet evts kept if Δφ<2.5); no isolated leptons. Main backgrounds: Z(→νν)+jets and W+jets – determined from data using Z(→μμ)+jets and W(→μν)+jets Paolo Rumerio, University of Alabama June 8, 2012 21

DM and LED PT leading jet and MET distributions after final event selection SM background prediction and comparison with data Paolo Rumerio, University of Alabama June 8, 2012 22

DM and LED 90% CL upper limits on dark matter-nucleon cross section for spin dependent and spin independent models – and comparison with direct detection limits 95% CL lower limits on fundamental mass scale MD of ADD model versus number of extra dimensions Paolo Rumerio, University of Alabama June 8, 2012 23

Search for Three-Jet Resonances (EXO-11-060) Paolo Rumerio, University of Alabama June 8, 2012 24

RPV decay of gluino excluded for masses Three-Jet Resonances Jet ensemble technique used to select jet-triplet combinations out of 6 selected high-pT jets Large signal combinatoric and SM multijet background Triplet mass distribution fit to functional form + a gaussian to set upper limits on the cross section Various extensions of SM predict resonances that decay into multi-jet states: Heavy colored fermions RPV decay of SUSY gluinos Benchmark model: gluino pair production, each decaying into 3 jets RPV decay of gluino excluded for masses 280 - 460 GeV Paolo Rumerio, University of Alabama June 8, 2012 25

Pair-Produced Di-Jet Resonances Searches for: Pair-Produced Di-Jet Resonances (EXO-11-016, 2.2 fb-1) Di-Jet Resonances using Di-Jet Angular Ratio (EXO-11-026, 2.2 fb-1) Paolo Rumerio, University of Alabama June 8, 2012 26

Di-Jet Resonance Searches (2.2 fb-1) Di-jet resonances using Δη ratio distrib. e.g. excited quarks → qg Pair-Produced di-jet resonances e.g. coloron → qq Excited quark mass exclusion < 3.2 TeV Coloron mass exclusion 320 - 580 GeV Paolo Rumerio, University of Alabama June 8, 2012 27

Conclusions Analyses based on jets and MET play an important role in searches for new physics New techniques (e.g. jet substructure) are being used with remarkable results Methods to deal with high pileup have proved to be effective The impressive performances of accelerator and experiment are making possible to continuously extend the range of the searches The data has reserved no surprises so far The search continues with the closing of the 2011 effort and – full steam – with the analysis of the 2012 dataset Paolo Rumerio, University of Alabama June 8, 2012 28

BACKUP Paolo Rumerio, University of Alabama June 8, 2012 29

Boosted tt - Systematics Exo11006 Paolo Rumerio, University of Alabama June 8, 2012 30

Boosted tt Likelihood fit to tt mass distribution 95% CL limit on σ x B.R. Extracted using CLs method Exo11006 Topcolor Z' excluded between masses of: 1.3-1.5 TeV for 1% width 1.0-1.6 TeV for 3% width 1.0-2.0 TeV for 10% width Randall-Sundrum Kaluza-Klein gluon excluded in 1.4-1.5 TeV and small region close to 1 TeV Counting technique poses a <2.6 limit on possible cross section enhancement w.r.t SM expectationfor tt mass > 1 TeV (a priori most probable value is 2.5) Limits on the possible cross section times branching ratio of ttbar resonances. This plot uses Z' sample with 1% width assumption. Limits on the possible cross section times branching ratio of ttbar resonances. This plot uses Randall-Sundrum Kaluza-Klein gluon samples. Paolo Rumerio, University of Alabama June 8, 2012 31

Boosted tt – Results Exo11006 Paolo Rumerio, University of Alabama June 8, 2012 32

RS G* → jet+MET XXX B A B A C D C D SM Bkg MG=1250 GeV k/MPl=0.05 Paolo Rumerio, University of Alabama June 8, 2012 33

RS G* → jet+MET Paolo Rumerio, University of Alabama June 8, 2012 34

G*/W' → VZ → qqll The results for the RS Graviton can be extended to other values of k/MPl assuming that the resonance width is much smaller than experimental resolution and the signal efficiency does not change Paolo Rumerio, University of Alabama June 8, 2012 35

Black Holes Total transverse energy (ST) distributions for low multiplicity (N=2, 3) events Paolo Rumerio, University of Alabama June 8, 2012 36

Black Holes Total transverse energy (ST) distribution for multiplicity N ≥ 6 events, and expected semiclassical BH signals Model-independent 95% CL limits on N ≥ 6 cross section for ST > STmin versus STmin Paolo Rumerio, University of Alabama June 8, 2012 37

Black Holes 95% CL cross section limits for counting experiments optimized for various BH parameters compared with signal cross sections vs. BH mass Paolo Rumerio, University of Alabama June 8, 2012 38

Black Holes Minimum BH mass excluded at 95% CL vs. reduced Planck scale MD for n=6 Cross section limits for various string ball parameters compared with signal production cross section vs. minimum string ball mass Paolo Rumerio, University of Alabama June 8, 2012 39