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Quark Compositeness Search with γ +Jet Final State at the LHC Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh Choudhary, Debajyoti Choudhury Department.

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Presentation on theme: "Quark Compositeness Search with γ +Jet Final State at the LHC Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh Choudhary, Debajyoti Choudhury Department."— Presentation transcript:

1 Quark Compositeness Search with γ +Jet Final State at the LHC Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh Choudhary, Debajyoti Choudhury Department of Physics & Astrophysics University of Delhi, India India-CMS Delhi 28 th September 2007

2 2 Outline Motivation for the Study Earlier studies within the same model Signal and Backgrounds Future Plans

3 3 Motivation Probes coupling of excited quark to its SM counterparts Physics at low luminosity (~100 pb -1 to 1 fb -1 ) Direct search for mass peak Limits can be set on parameter space much above the Tevatron reach Di-jet QCD background is reducible due to clean hard photon (with tight isolation cuts)

4 4 Earlier Work with Di-photon Final State arXive: v1[hep-ph] CMS IN 2007/039 Submitted to PRD (responding to referees comments)

5 5 Poster Presented at Lepton Photon 2007, Daegu, Korea SELECTED AS BEST POSTER IN EXPERIMENTAL PARTICLE PHYICS CATEGORY CERTIFICATE & PRIZE AWARDED

6 6 Signal and Backgrounds  Feynman diagrams for the γ+jet background (Type-I).  Z(jj)+γ and W(jj)+γ Background (Type-II).  Feynman diagrams for the signal. Mass Peak No Peak, Excess over SM part

7 7 Matrix Element for qg  γ +Jet via q* SM Piece By: Prof. Debajyoti Choudhury

8 8 Background and X-sections Pt – hat GeV GeV GeV GeV GeV GeV >1500 GeV qg x x x10 -4 qqbar x x x x10 -4 gg x x x x x x10 -9 Cross Section (pb) for backgrounds in different P T -hat bin Type-1: SM γ+jet Background – Non-Reducible Interested above 200 GeV onwards.

9 9 Background and X-Section Pt –hat GeV GeV GeV GeV GeV GeV >1500 GeV Z(jj)+ γ x x x x x X10 -6 W(jj)+ γ x x x x x x10 -6 Type-2: From Z(jj)+  & W(jj)+  - small & reducible but comparable to gg  γ+jet) Type-3: SM Jet-Jet background where one of the Jet(s) fakes a Photon – Largest Background – Reduce with isolation requirements

10 10 Photon and Jets Algorithm to “reconstruct” the photon at the generator level (Reference - Marco Pieri et al. CMS IN 2005/018, and CMS IN 2007/039 – our earlier study)  Select a seed with P ,e± T > 5 GeV  Search around the seed in 10x10 crystal geometry in φ and η directions  With Δφ=0.09 and Δη=0.09  Add 4-momentum vectors of found EM objects  Vector additions provides Photon Candidate  For Jet used Iterative Cone Algorithm with R=0.5 and seed P T  1.0 GeV (Inclusive jet i.e. neutrinos and muons are included in the jet definition)

11 11 Preliminary Distributions (I) Generation cuts: P T -hat ≥ 190 GeV on partons with no cut on η All plots are for L int =10 pb -1 Signal is qg  γ+jet via q*

12 12 Preliminary Distributions (II) Selection Cuts: P Tγ ≥ 200GeV, P T jet ≥200 GV | η γ | ≤ 2.5, |η jet | ≤ 2.5

13 13 Preliminary Distribution (III)

14 14 Preliminary Distribution (IV)

15 15 Preliminary Distribution (V) Backgrounds and signal separately Invariant Mass distribution without any isolation cuts

16 16 Preliminary Distribution (VI) Isolation variables: To decide track minimum P T to count them as track (final state, pi ±, e ±, p ± & K ± are considered as tracks )

17 17 Preliminary Distribution (VII) With Isolation cut: R iso ≤ 0.35, E T SUM < 5GeV Study in progress to understand other isolation variables such as – number of tracks etc. and optimize various isolation cuts

18 18 Future Plans Complete the generator level study for q* to γ +jet final state with large statistics and set limits on Λ and Mq* for CMS setup (Submit as CMS IN) This study will be presented in the SUSY/BSM meeting on 28 th September at CERN At present interfacing γγ and γ +Jet final states via q* within CMSSW framework as an external routine. Will soon provide.cfg file for both channels to the production team.

19 Thank you!

20 20 Backup Slides

21 21 Available Literature For Quark & Lepton compositeness: Dijet channel ( Phys.Rev. D-03110, Robert Harris hep- ph/ ) Drell -Yan (S. Jain et. al.hep-ex/ ) Gamma+Jet final State: ATLAS collaboration ( ATL –PHYS ). ( No such study exists for CMS) Two photon final state: Some phenomenological studies have been done without complete SM background e.g., Thomas G. Rizzo PRD v51,Num-3 ( No such study exists for CMS )  Existing Limit at the LHC’s center of mass energy, with two photon final state is: ~Λ >2.8 TeV for contact interaction (depends on kinematical cuts and luminosity)

22 22 Compositeness scale Compositeness scale: Λ >> sqrt (s-hat) : Contact interaction Λ << sqrt (s-hat) : Excited state Λ ~ sqrt (s-hat) : Model Dependent

23 23 Present Limit on M* –CDF: M* > 80 GeV (q*  q  ) –CDF: M* > 150 GeV (q*  q W ) –CDF (All channels): M* >200 GeV –D0 : M*> 200 GeV Simulation study: Mass reach up to 0.94 TeV at Tevatron ( 2 TeV, 2 fb -1, q*  q-qbar) ATLAS Study: upto 6.5 TeV at LHC ( f=f s =1, q*  q  ) Limits from Tevatron:


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