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Search For the Higgs o H ->ZZ*->bbll Philip Davis (NMSU) Mentor: Dr. Teuscher (U of T) Aided by Christophe Le Maner (U of T) Invariant Mass of Higgs for mH of 150 GeV before Cuts Electron (shown) and Muon System Luminosity 30 fb-1 Mass Analysis on mH of 150 GeV Higgs Signal Back Grounds tt ZZ Zbb bb Zee Zmm Intro Previous analysis of this decay channel done by Christophe Le Maner Monte Carlo Data created using Pythia, MCatNLO, and AcerMC New Monte Carlo Data simulated after first analysis What I did Try to recreate old analysis Apply my own analysis Create automated system of applying cuts Cuts for mH of 150 GeV on Electron Channel (Previous Analysis) Cut Value Zero total charge on lepton pair Charge e1 + e2 = 0 Inv. Mass of Virtual Z System 10 < mZ < 65 GeV Inv. Mass of Z System 50 < mZ < 110 GeV η1 and η2 of VBF jets opposite dir. η1*η2 < 0 Diff. in pseudo rapidity of VBF jets |∆η| > 3.3 Mass of VBF jets mjj > 300 GeV Missing Pt Ptmiss < 25 GeV b jet and lepton in between VBF jets Mass window 130 < mH < 170 GeV Previous Analysis Higgs Mass S S/√BG H130 (ee channel) 0.14 0.057 H150 (ee chanel) 0.79 0.227 H130 (μμ chanel) 0.13 0.052 H150 (μμ chanel) 0.75 0.18 - Christophe Le Maner Repeating Previous Analysis Higgs Mass S S/√BG Relative Error H130 (ee channel) 0.246 0.025 25.88% H150 (ee chanel) 0.901 0.0812 20.63% H130 (μμ chanel) 0.209 0.027 33.59% H150 (μμ chanel) 0.877 0.0938 25.10% (New Data) Cuts for mH of 150 GeV on Electron Channel Cut Value 2 b-jets required Invariant mass of di-electron System Missing Pt Diff. in pseudo rapidity of VBF jets Sum of Pt of VBF Jets Mass of VBF jets 10 < mee < 65 GeV Pt < 25 GeV |∆η| > 3.3 Pt 1 + Pt 2 > 90 GeV mjj > 300 GeV η1 and η2 opposite dir. η1*η2 < 0 Inv. Mass of Z System 50 < mZ < 110 GeV Zero total charge on lepton pair Charge e1 + e2 = 0 Mass window 130 < mH < 170 GeV Histograms Gev • 50 < mzo < 110 GeV •10 < mee < 65 GeV •(constrain leptons to come from Virtual Z) More Histograms GeV Missing Pt < 25 GeV GeV Mass of VBF jets > 300 GeV Pt of Forward Jet 1 Vs. Jet 2 Sum > 90 GeV Pt of 2 jet (GeV) Pt of 1 jet (GeV) New Cuts Higgs Mass S S/√BG Relative Error H130 (ee channel) 0.232 0.0339 39.57% H150 (ee chanel) 0.882 0.103 28.23% H130 (μμ chanel) 0.207 0.032 41.64% H150 (μμ chanel) 0.878 0.116 31.13% •Problem with H130 data is that it start out with low number of events •Increase in S/√BG from old cuts •Increase in Relative Error from old cuts •H150 data gives better results but still low significance •Signal Rejection ~ 21% (H150 ee chanel) •Background Rejection ~ 0.028% (H150 ee chanel) Signal after Cuts Higgs Signal Fully Automated Cut System Program run cuts over a range of values and stores results to root file. Results searched my another program to return cuts with best outputs. Only used old data on this program. Relative Error usually about 100% Next step should be to uses this method on new data Protection Circuit for LVPS Background Front end electronics of the Tile Calorimeter in ATLAS are kept in drawers as seen above. TileCal has 256 of these drawers Each drawer requires its own power supply. Background/Problem The Low Voltage Power Supply (LVPS) converts a 200 V DC power supply to 8 DC voltages required by the front end electronics in the TileCal. When installed in the pit the LVPS has burned up components due to voltages going over their ratings. Important issue for LHCC Solution Regulating Circuit that monitors the 8 voltages and currents going to the detector. Monitors for under-voltage, over-voltage, and over-current. Circuit switches power off in TileCal when voltage or current goes out of range. Voltages put into two groups. High Voltage side and Digitizer side. High Voltage When one side is triggered the other side can still operate. Circuit Simulation Circuit simulated in Quartus II Implemented in Embedded Local Monitor Board (ELMB) in the LVPS Circuit Explanation Current input Voltage input Trip Outputs 32 bit Shift Register Redundancy circuit Wave form of Inputs and Outputs Outputs of Digitizer and High Voltage Trigger Output of Shift Register Special Thanks Dr. Teuscher Christophe Le Maner CERN University of Michigan NSF Ford Backup slides Cut Table Cuts with weights for Electron Channel Cut mH tt Zbb ZZ Zee Zmm bb Total BG Total number of events 4.19315 41968.3 19334.4 64.86 8802.7 8911.03 176032 number of bjets 3.92187 40309.1 18031.2 59.891 8723 0 117355 invariant mass of electrons 2.63913 16928 1034.99 7.46192 55.3264 0 9338.7 missing pt 2.05103 1380.35 815.202 5.61553 49.5229 0 0 Delta of eta for VBF jets 2.05103 1380.35 815.202 5.61553 5.41657 0 0 sum pt of vbf jets 1.35695 481.919 245.217 0.517659 0.386898 0 0 mass of vbf jets 1.32322 441.759 218.973 0.436551 0 0 0 eta1*eta2<0 1.32322 441.759 218.973 0.436551 0 0 0 zed mass 1.09917 115.89 91.0336 0.34113 0 0 0 even charge 1.0972 102.121 90.2135 0.331588 0 0 0 mass window 0.881866 33.2754 39.3659 0.0978065 0 0 0 Signal/sqrt(BG) 255113 184478 47364.4 2250.7 2206.59 728.041 661.169 661.169 207.265 192.666 72.7391 0.00830183 0.00913106 0.0121265 0.0432329 0.0436628 0.0502907 0.0514607 0.0514607 0.0763487 0.0790467 0.1034 Cuts with weights for Muon Channel Cut Total number of events Total number bjets invariant mass of muons missing pt Delta of eta for VBF jets sum pt of vbf jets mass of vbf jets eta1*eta2<0 zed mass even charge mass window mH 3.62164 3.39871 2.29167 1.97626 1.97626 1.31479 1.28302 1.28302 1.07471 1.07415 0.87793 tt 37159.4 35726.3 13948.1 1040.72 1040.72 346.523 316.69 316.69 81.4673 78.025 19.5063 Zbb 15123.9 14185.7 773.376 666.76 666.76 223.073 209.131 209.131 83.6525 83.6525 37.7256 ZZ 48.7148 45.2463 5.44377 4.52534 4.52534 0.527201 0.474719 0.474719 0.372142 0.372142 0.145517 Zee 8802.7 0 0 0 0 0 0 0 0 0 0 Zmm 8911.03 8818.64 6.70331 4.66317 0.874345 0 0 0 0 0 0 bb 176032 58677.3 29338.7 29338.7 0 0 0 0 0 0 0 Total BG 246078 117453 44072.3 31055.3 1712.88 570.124 526.296 526.296 165.492 162.05 57.3774 Signal/sqrt(BG) 0.00730077 0.00991704 0.0109161 0.0112144 0.0477508 0.0550644 0.0559266 0.0559266 0.0835418 0.0843803 0.115902 Output of HV and Digitizer Pins Wave of output pins Shows that each input works and that the corresponding output pin is triggered.