Kohei Yorita Young-Kee Kim University of Chicago

Slides:



Advertisements
Similar presentations
STAR Status of J/  Trigger Simulations for d+Au Running Trigger Board Meeting Dec5, 2002 MC & TU.
Advertisements

UK egamma meeting, Sept 22, 2005M. Wielers, RAL1 Status of Electron Triggers Rates/eff for different triggers Check on physics channels Crack region, comparison.
H/Abb -> 4b’s process & Multi-Et-Threshold Study for 4jet Trigger Kohei Yorita Young-Kee Kim University of the FTK Meeting on July 13 th, 2006.
 Trigger for Run 8 Rates, Yields, Backgrounds… Debasish Das Pibero Djawotho Manuel Calderon de la Barca Analysis Meeting BNL October 16, 2007.
Skeleton outline for the physics case document M. Shochet December 15, 2005.
1  trigger optimization in CMS Tracker Giuseppe Bagliesi On behalf of  tracking group Workshop on B/tau Physics at LHC Helsinki, May 30 - June 1, 2002.
FTK Studies: H  hh  bbbb FTK Physics Case Meeting 11/03/05 Erik Brubaker University of Chicago.
FTK Production on UC Tier3 and Hidden Valley Processes Jan 23, 2007 Erik Brubaker FTK meeting.
September 27, 2005FAKT 2005, ViennaSlide 1 B-Tagging and ttH, H → bb Analysis on Fully Simulated Events in the ATLAS Experiment A.H. Wildauer Universität.
Progress on the FTK Physics Case (For H/Abb 4b signal) Kohei Yorita Young-Kee Kim University of FTK Meeting on January 26 th, 2006 (1)Brief Sample.
Progress on H/Abb -> 4b’s channel for the FTK physics case ~ 4jets trigger w/ and w/o FTK ~ Kohei Yorita Young-Kee Kim University of the FTK.
Daniele Benedetti CMS and University of Perugia Chicago 07/02/2004 High Level Trigger for the ttH channel in fully hadronic decay at LHC with the CMS detector.
Update on Tools FTK Meeting 06/06/06 Erik Brubaker U of Chicago.
Update on H/Abb -> 4b’s process (4jet Trigger) Kohei Yorita Young-Kee Kim University of the FTK Meeting on Sep. 7 th, 2006.
Sept 30 th 2004Iacopo Vivarelli – INFN Pisa FTK meeting Z  bb measurement in ATLAS Iacopo Vivarelli, Alberto Annovi Scuola Normale Superiore,University.
July 20, 2005S.Abdullin SUSY Triggers1 Salavat Abdullin For CMS Collaboration SUSY 2005, July 18-23, 2005 Durham, UK.
Update FTK Meeting 07/13/06 Erik Brubaker U of Chicago.
1 A Feasibility Study for a Strange Sea Asymmetry Analysis at ATLAS: update II Laura Gilbert and Jeff Tseng 13/12/07.
Progress on B-tagging Efficiency Monica Dunford May 22 nd, 2007.
1 Viktor Veszprémi (Purdue University, CDF Collaboration) SUSY 2005, Durham Search for the SM Higgs Boson at the CDF Experiment Search for the SM Higgs.
Status Report on hbb Analysis Jyothsna Rani for the hbb group Andy, Avto, Marine, Tim, Boris All D0 Meeting 28 th January th January 2005.
H  FTK update Catalin, Tony FTK meeting, 9/7/2006.
Update on H  studies Catalin and Tony FTK meeting, July 13, 2006.
FTK update H→  Tony, Catalin By speeding up/adding rejection at LVL2, we can have a higher rate coming in from LVL1. Therefore some of the LVL1 threshold.
Update Apr 24, 2007 Erik Brubaker FTK meeting. April 24, 2007FTK Meeting2 LVL1/LVL2 jet triggers Set trigger thresholds according to TDR scheme. E.g.,
Dijet Mass Sherpa vs Pythia Multi-Threshold e.t.c. for H/Abb->4b’s Kohei Yorita University of Chicago FTK Meeting 12/19/2006.
Update FTK Meeting 05/02/06 Erik Brubaker U of Chicago.
E. Devetak - LCWS t-tbar analysis at SiD Erik Devetak Oxford University LCWS /11/2008 Flavour tagging for ttbar Hadronic ttbar events ID.
Associated top Higgs search: with ttH (H  bb) Chris Collins-Tooth, 17 June 2008.
1 2vtx tagged diBjets mass cross section measurement Univeristy of Notre Dame Hong Luo Mar 3 th 2005.
Future  G Measurements at STAR Renee Fatemi University of Kentucky RHIC Spin Meeting, LBNL, November 21st 2009.
Progress on H/Abb -> 4b’s channel for the FTK physics case ~ 4jets Trigger w/ and w/o FTK ~ Kohei Yorita Young-Kee Kim University of the FTK.
Selection cuts on Bs→ with FTK F. Crescioli, P. Giannetti, M. Dell'Orso, G. Punzi, G. Volpi 2/5/2006.
Commissioning Studies Top Physics Group M. Cobal – University of Udine ATLAS Week, Prague, Sep 2003.
HERA-LHC, CERN Oct Preliminary study of Z+b in ATLAS /1 A preliminary study of Z+b production in ATLAS The D0 measurement of  (Z+b)/  (Z+jet)
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
Possibility of tan  measurement with in CMS Majid Hashemi CERN, CMS IPM,Tehran,Iran QCD and Hadronic Interactions, March 2005, La Thuile, Italy.
1 TTU report “Dijet Resonances” Kazim Gumus and Nural Akchurin Texas Tech University Selda Esen and Robert M. Harris Fermilab Jan. 26, 2006.
Study of Standard Model Backgrounds for SUSY search with ATLAS detector Takayuki Sasaki, University of Tokyo.
Simone Gennai SNS, INFN-Pisa1 Radion searches in CMS A first look to  hh G. Dewhirst, L. Fano, S. Gennai, S. Nikitenko.
Physics at LHC Prague, 6-12 July, 2003 R. Kinnunen Helsinki Institute of Physics A/H ->  and H + ->  in CMS R. Kinnunen Physics at LHC Prague July 6.
M. Pilar Casado 1 Optimization of Tau Menus: L1 & L2 Trigger & Physics week (19-22 March 2007) M. Pilar Casado (IFAE & UAB) on behalf of the Tau Trigger.
STAR J/  Trigger in dA Manuel Calderon for the Heavy-Flavor Group Trigger Workshop at BNL October 21, 2002.
Study on search of a SM Higgs (120GeV) produced via VBF and decaying in two hadronic taus V.Cavasinni, F.Sarri, I.Vivarelli.
1 Update on tt-bar signal and background simulation Stan Bentvelsen.
Flavour independent neutral Higgs boson searches at LEP Ivo van Vulpen NIKHEF On behalf of the LEP collaborations EPS conference 2005.
1 Jet Triggers and Dijet Mass Selda Esen and Robert M. Harris Fermilab TTU Weekly HEP Group Meeting Feb 16, 2006.
Charged Particle Multiplicity, Michele Rosin U. WisconsinQCD Meeting May 13, M. Rosin, D. Kçira, and A. Savin University of Wisconsin L. Shcheglova.
A search for the ZZ signal in the 3 lepton channel Azeddine Kasmi Robert Kehoe Southern Methodist University Thanks to: H. Ma, M. Aharrouche.
La Thuile, March, 15 th, 2003 f Makoto Tomoto ( FNAL ) Prospects for Higgs Searches at DØ Makoto Tomoto Fermi National Accelerator Laboratory (For the.
Mark OwenManchester Christmas Meeting Jan Search for h ->  with Muons at D  Mark Owen Manchester HEP Group Meeting January 2006 Outline: –Introduction.
1 UCSD Meeting Calibration of High Pt Hadronic W Haifeng Pi 10/16/2007 Outline Introduction High Pt Hadronic W in TTbar and Higgs events Reconstruction.
Viktor Veszpremi Purdue University, CDF Collaboration Tev4LHC Workshop, Oct , Fermilab ZH->vvbb results from CDF.
VHF working meeting, 4 Oct Measurement of associated charm production in W final states at  s=7TeV J. Alcaraz, I. Josa, J. Santaolalla (CIEMAT,
Update on Invisible Higgs analysis in the tth channel
More technical description:
Muons from single top events for DC04
ttH (Hγγ) search and CP measurement
Venkat Kaushik, Jae Yu University of Texas at Arlington
Philippe Doublet, LAL Roman Pöschl & François Richard, LAL
Higgs → t+t- in Vector Boson Fusion
Hidden Valley Processes
tt+jets simulation comparisons
Erik Brubaker U of Chicago
Di-jets & MT2 for early SUSY discovery
Physics Studies Update
Search for supersymmetric neutral Higgs bosons in the decay channel A/H->m+m- in the ATLAS detector George Dedes , Sandra Horvat Max-Planck-Institut.
Muons from light meson decays
Higgs  update Catalin and Tony May 22, 2007
Experimental and theoretical Group Torino + Moscow
Presentation transcript:

Progress on H/Abb -> 4b’s channel for the FTK physics case ~ 4jets trigger w/ and w/o FTK ~ Kohei Yorita Young-Kee Kim University of Chicago @ the FTK Meeting on May 2nd, 2006

Trigger Rate Comparisons > Requiring 4jets with different Pt cuts. > Trigger Rate : Sherpa 2to3 > Sherpa 2to2 > Pythia > No bb production in Sherpa but gluon splitting produces b quarks. bb production : 0.48 mb with no pt cut ~ 0.002 mb with pt>20 GeV, < 1% w.r.t. dijet - Need more check. > Use Sherpa 2to3, yt>25 as a default - Better kinematics and conservative. Sample Xsec(mb) NEV Sherpa2to3, yt>20 0.827 ~11M Sherpa2to3, yt>25 0.361 Sherpa2to2, yt>20 0.776 ~9.4M Sherpa2to2, yt>25 0.340 ~1M PYTHIA dijet, pt>20 0.817 300K 1 btag 2 btag 0 btag 3 btag 4 btag

Atlfast Pt vs LVL1 8x8 Calo Et Old : |eta| < 2.8, JETB New : |eta| < 3.2, against both JET and JETB (option) > Slope became more closer to 1, and turn-on curve gets more steeper. In TDR, LVL1 Pt is set to 55-65 GeV, That corresponds to 35-45 GeV 8x8 Calo Cluster Et, giving ~100Hz of LVL1 output rate. Due to yt>25 cut, rates in lower pt region might not be true. (unlikely to have 2KHz by 10 GeV of LVL1 8x8 Calo cluster Et.) Not exactly sure what’s happening. - need more investigation. For this talk, everything is based on Atlfast Pt. TDR 4jets w/o btag

How Much Can We Lower the Pt Threshold at LVL1 ? Assume that a realistic limit of LVL1 output rate for our jet trigger is a few KHz in the default table. (total 40 -> 100 KHz) This limits lowering threshold rather than LVL2 reduction rate with FTK. LVL1 : To give ~1KHz of LVL1 output, Pt threshold for 4jets is ~40 GeV. TDR : Pt>55-65 GeV, ~200Hz. LVL2 : In any case LVL2 output has to be an order of ~10Hz. TDR : Pt>90-110 GeV, ~10-20Hz. So trying to keep 40GeV even @ LVL2 and reduce LVL2 output rate to ~10Hz by only requiring btagging. 1 btag 2 btag 3 btag 4 btag

LVL2 Reduction by btagging Due to contents of b quarks, The reduction rate is not simple linear dependency w.r.t. Ru (light jet rejection factor). - Compare dotted lines with solid lines Why is real reduction rate higher than slope of 1 ? (1) 4jets with |eta| < 3.2 (2) 4jets with |eta| < 2.5 & N-btag So eff. of N(eta<2.5)/N(eta<3.2) is included. Denominator : N(eta<2.5) * Need to check bb production.

Setting up working points for the cases w/ and w/o FTK Conditions to be considered : (1) Pt cut @ LVL1 can not be lowered below 40 GeV (limited by LVL1 output rate) (2) Pt cut @ LVL2 can be changed by requiring btag. But it has to give the same LVL2 rate as Pt>110 GeV w/o btag (TDR) A ~10Hz LVL1 LVL2 A 4J 55-65 : rate ~200Hz 4J110 no btag : output rate 9.6 Hz B 4J40 : rate ~1KHz 4J40 w/ 1btag, Ru=100 : output rate 13.4 Hz C 4J40 w/ 2btag, Ru=10 : output rate 6.5 Hz w/o FTK B C w/ FTK LVL1 limit

Trigger Rate vs Signal Efficiency 4J110 no btag B 4J40 w/ 1btag, Ru=100 C 4J40 w/ 2btag, Ru=10 In each line from right to left, each point comes from 20,30,40, …….. GeV Pt cut. 20 1 btag 2 btag 30 40 50 A(110) A B(40) C(40) Signal acceptance is increased by a factor of 10-20 by btagging, while keeping LVL2 output rate around 10Hz !

Improvement at Trigger Level 4J110 no btag B 4J40 w/ 1btag, Ru=100 C 4J40 w/ 2btag, Ru=10 Btagging efficiency : 50% @ L = 30 fb^-1 MA Signal Eff. (%) S B (LVL2 out rate) S/B (%) S/sqrt(S+B) 300 (39.9pb) A 0.24 2884 1.44e+8 (9.6Hz) 2.0e-3 B 4.51 53936 2.01e+8 (13.4Hz) 2.7e-2 3.80 C 2.02 24223 9.82e+7 (6.5Hz) 2.5e-2 2.44 500 (4.18pb) 1.12 1404 9.7e-4 0.12 9.67 12127 6.0e-3 0.86 4.24 5317 5.4e-3 0.54 700 (0.82pb) 2.86 704 4.9e-4 0.06 13.6 3349 1.7e-3 5.95 1464 1.5e-3 0.15 900 (0.21pb) 5.61 353 2.5e-4 0.03 16.6 1044 5.2e-3 0.07 7.28 458 4.7e-3 0.05

Optimization to see (Final) Improvements w/ and w/o FTK Since optimization can be done in offline, (i.e. using offline quality btag), Only difference between w/o and w/ FTK is 4th jet pt threshold (110 and 40 GeV) - Looked at up to (300,200,120,120), 10 GeV step and up to 4 btags. A (w/o FTK) Eff_b = 50%, Eff_c = 10%, mistag 1%, Start from 4J110 B (w/ FTK) Eff_b = 50%, Eff_c = 10%, mistag 1%, Start from 4J40 @ L = 30 fb^-1 MA Optimized cuts S B S/B (%) S/sqrt(S+B) 300 A(140,140,110,110), +4b 62.9 13.9 451 7.17 B(130,70,70,40), +4b 1175 1352 86.9 23.4 500 A(160,140,110,110), +4b 29.9 12.9 231 4.6 B(160,120,70,40), +4b 251 489 51 9.2 700 A(220,130,110,110), +4b 11.4 9.9 115 2.5 B(290,200,40,40), +3b 200 1122 17.8 5.5 900 5.1 1.3 B(300,200,40,40), +3b 94 1043 9.0 2.8 Optimized by S/sqrt(S+B), not very stable due to low stat and tight cuts.

Very Quick Look w/o FTK w/ FTK *** Note *** This is very preliminary & optimistic, because there is no bb production taken into account. And also signal cross section used is slightly larger than TDR. Need more study to say something conclusive. But relative improvement looks very nice and promising. 700

Summary > By requiring high quality btagging by FTK at LVL2, we can lower the pt threshold to 40 from 110 GeV while keeping ~10Hz of LVL2 output rate and ~1KHz of LVL1 output. > At Trigger level, this gives significance improvement by a factor of 2-10. > After optimization, we still do see good improvement with FTK. Statistical significance gets better by a factor of 2-3 depending on MA. Things to do : > Should look at dijet mass distributions. > Need more careful study on LVL1 parameterization. > Need to look at bb production in Sherpa. > Need Ru vs btag efficiency plot from realistic FTK simulation. > Plan to look at full simulation for signal. > Make conclusions : - How much can tan be improved (lowered) in this channel ? - Can we measure the mass of Higgs by having FTK ? > Documentation.

With Other Final States Obviously 4b channel is not discovery channel But need it for property !