Single Top At Hadron Colliders

Similar documents
La ricerca dell Higgs Standard Model a CDF

The Tevatron s Search for High Mass Higgs Bosons

Physics at Tevatron. Koji Sato KEK Theory Meeting 2005 Particle Physics Phenomenology March 3, Contents

Evidence for Single Top Quark Production. Reinhard Schwienhorst

Single top: prospects at LHC

Recent Results from the Tevatron

Physics at Hadron Colliders

Top Physics at CMS. Intae Yu. Sungkyunkwan University (SKKU), Korea Yonsei University, Sep 12 th, 2013

ATLAS Discovery Potential of the Standard Model Higgs Boson

Top and Electroweak Physics at. the Tevatron

Pedro Teixeira-Dias. Higgs Overview

Highlights of top quark measurements in hadronic final states at ATLAS

Search for the Standard Model Higgs in WW (lν)(lν)

Measurement of t-channel single top quark production in pp collisions

Inclusive top pair production at Tevatron and LHC in electron/muon final states

NEW RESULTS FROM THE TOP QUARK

SUSY Phenomenology & Experimental searches

Single-Top at the Tevatron

Top quark at LHC. M. Villa. Bologna, oggi

B-quark discovery. e+ e- PETRA GeV TRISTAN 61.4 GeV LEP Mz Mt > 45.8 GeV

Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production.

Measurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay

Preparations for SUSY searches at the LHC

Search for SUSY at CMS in lepton or photon final states. PANIC 2011 K. Theofilatos (on behalf of CMS)

Title Text. ATLAS Higgs Boson Discovery Potential

Searching for the Higgs at the Tevatron

arxiv: v1 [hep-ex] 27 Nov 2017

Searches for Standard Model Higgs Boson at the D Detector at the Tevatron. Alexander Khanov Oklahoma State University SUSY 06

Preparations for SUSY searches at the LHC

Combination of top quark physics results at the LHC

W/Z + jets and W/Z + heavy flavor production at the LHC

Top production measurements using the ATLAS detector at the LHC

ZZ 4l measurement with the first ATLAS data

Recent Results on Top Physics at CMS

Recent Results from CDF. Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration

Top Physics in Hadron Collisions

SUSY Search Strategies at Atlas and CMS

Pursuing EWK Symmetry Breaking at CDF

CDF top quark " $ )(! # % & '

Some Thoughts on What Else to Trigger with the FTK

Ernest Aguiló. York University

Studies of top pair production in the fully hadronic channel at LHC with CMS

Progress in Top Quark Physics

Evidence for s-channel single top production at DØ

Top quark pair cross section measurements at the Tevatron experiments and ATLAS. Flera Rizatdinova (Oklahoma State University)

Higgs Boson Searches at ATLAS

Top physics at CDF. Journal of Physics: Conference Series. Related content

Z boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011

arxiv: v1 [hep-ex] 8 Nov 2010

Study of Higgs boson leptonic decay modes

Top production at the Tevatron

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CEA-Saclay, IRFU/SPP, bât. 141, Gif sur Yvette Cedex, France On Behalf of the CDF and DO Collaborations.

NEWS FROM THE TOP. 1. Pair Production of Top Quarks Cross Section Search for Resonances Forward-Backward Asymmetry

From Precision Electro-weak Physics to Beyond-the-SM Physics Searches

Discovery potential of the SM Higgs with ATLAS

Jet Substructure. Adam Davison. University College London

Direct measurement of the W boson production charge asymmetry at CDF

Searches at the LHC: Results from first data

Tobias Golling - SCIPP - August 24th 2004

SEARCH FOR 4 TH GENERATION QUARKS AT CMS

Search for tt(h bb) using the ATLAS detector at 8 TeV

First two sided limit on BR(B s μ + μ - ) Matthew Herndon, University of Wisconsin Madison SUSY M. Herndon, SUSY

W/Z+jet results from the Tevatron

The Top Quark Mass in the Muon+Jets Final State at s = 13 TeV in 2015 Data

Don Lincoln. QCD Results from the Tevatron

Measurement of the Top quark mass

Results on top physics by CMS

Extra dimensions and black holes at the LHC

QCD Multijet Background and Systematic Uncertainties in Top Physics

HIGGS Bosons at the LHC

Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations

Prospects for Higgs Searches at CDF in Run II

ATL-PHYS /08/99

Single top quark production at CDF

QCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration

Measurements of the tt Cross Section and Top Mass at CDF

Combined Higgs Searches at DZero

PoS(DIS 2010)190. Diboson production at CMS

Top results from CMS

Strategies for b-tagging performance using t t events at CMS

Search for the Higgs boson in the t th production mode using the ATLAS detector

Contact the LHC

8.882 LHC Physics. Higgs Physics and Other Essentials. [Lecture 22, April 29, 2009] Experimental Methods and Measurements

Studies of Top Quark properties at the LHC. Top quark physics. S. Bentvelsen NIKHEF Kruislaan SJ Amsterdam the Netherlands

Stop NLSPs. David Shih Rutgers University. Based on: Kats & DS ( ) Kats, Meade, Reece & DS ( )

Search for a heavy gauge boson W e

First physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations

Two Early Exotic searches with dijet events at ATLAS

Why I never believed the Tevatron Higgs sensitivity claims for Run 2ab Michael Dittmar

First studies towards top-quark pair. dilepton channel at s = 13 TeV with the CMS detector

Higgs search in WW * and ZZ *

Boosted Top Resonance Searches at CMS

Beyond the Standard Model searches with top quarks at D0

Stating the Case for Top at the LHC

Standard Model Higgs Searches at the Tevatron (Low Mass : M H ~140 GeV/c 2 )

Higgs-related SM Measurements at ATLAS

Search for W' tb in the hadronic final state at ATLAS

Latest results on the SM Higgs boson in the WW decay channel using the ATLAS detector

The Higgs boson discovery. Kern-und Teilchenphysik II Prof. Nicola Serra Dr. Annapaola de Cosa Dr. Marcin Chrzaszcz

Transcription:

Single Top At Hadron Colliders Simona Rolli Tufts University

Overview Searches for single top at the TeVatron Current status Beyond 1 fb expectations Single Top at LHC (ATLAS) Analysis strategies Current activities Outlook for 100pb and full statistics A couple of phenomenology remarks in single top physics Conclusions 2

Top production modes Strong Interactions:tt pair Dominant mode: σ NLO+NLL = 6.7 +0.7-0.9 pb (TeVatron)) Signature understood (top discovery 1995) Weak Interactions: single top Larger background, smaller cross section Not yet observed at the TeVatron, observable at LHC 3

Why Single Top? M(top) = 175 GeV/c 2 s-channel t-channel Associated tw Combined (s+t) TeVatron σ NLO 0.88 ± 0.11 pb 1.98 ± 0.25 pb 0.1 pb LHC σ NLO 10.6 ± 1.1 pb 247 ± 25 pb 62 +17-4 pb Run I 95% CL CDF <18 pb < 13 pb D0 < 17 pb < 22 pb σ t+s = 2.9 pb for m(top) = 175 GeV/c 2 NA NA < 14 pb 4

Single Top at the TeVatron Signatures and Backgrounds 1/10 Analysis strategies CDF- separate channels search (2D NN) and combined channels search (1D NN and likelihood function compared to 2 hypothesis) D0 - separate channels search (likelihood discriminant method) 5

TeVatron Current Results (I) 370 pb -1 Study of variables having discriminating power against W + jets/ttbar (Qηfor example) ; Design of several likelihood discriminants for S/B separation; Combination of likelihoods in 2D histos; Extraction of limit 95% C.L. Upper Limit t-channel σ < 4.4 pb s-channel σ < 5.0 pb 6

TeVatron current results (II) Separate channels search 695 pb -1 Expected Data Likelihood fit is applied to the output of the 2D NN: t-channel: σ < 3.1 pb @ 95% C.L. s-channel: σ < 3.2 pb @ 95% C.L. Combined Channels (s+t) Upper Limit σ < 3.4 pb @ 95% C.L. 7

TeVatron outlook 8

Single Top at LHC 1 leptons + MET + 2 jets + 1(2) b-tags 9

ATLAS analysis strategies In the late 90 several studies were conducted to produce a physics TDR. Current studies are meant to devise analysis strategies for first data (100 pb -1 ) and the full statistics, using the latest software tools. 10

Wg channel 11

s-channel 12

Wt channel 13

Top Physics for Commissioning Current Activities 14

Current Activities Fast Simulation vs Full Simulation Require at least 1 electron p T > 30 GeV Light jets b jets All evts 40000 1 lepton 12178 1 b jets pt 50 6788 2 light jet pt 30 2873 (7.1%) 32028 evts with 1 one P T ele (XRatio > 0.6) 28582 evts with MET > 20 GeV 12175 evts with 1 and only 1 b-jet (Lhsig > 0.9, E T > 50, η < 2.5) 1566 evts with 2 jets (3 total) E T > 30, η < 2.5 2.4% final acceptance (3% TDR) 15

Current Activities (II) b-tagging efficiencies ε= ~50% Several algorithms in testing phase LHSig shown Efficiencies as function of cut and P T and η P T > 50 GeV 16

Current Activities (III) Systematic uncertainty Calorimeter resolution on/off smearing 17

Phenomenology Work Angular correlations in single top and Wjj production (NLO) They can be reliably predicted for both single top production and Wjj. Using fully correlated angular distribution a set of cuts is devised 18

Phenomenology Work Using charge asymmetry to measure single top production LHC is a gluon collider tt goes up, tbq goes up, W+jets only somewhat, tb very little ttbar really will be the dominant background It has been that showed jet veto can reduce tt enough to study single top in single tag channel (hep-ph/9807340) But jet veto was not enough to study single top in double b-tagged sample Charge asymmetries eliminate tt more effectively than jet vetos, allowing both single-tag and double-tag single top samples to be studied s-channel and t-channel both have cross-sections with charge asymmetries A C ~ 0.25 Wt channel not affected (b and bbar PDF are assumed to che charged-symmetric) W+jets remains the main source of background. A C = N N + +! + N N!! Δ: N + - N - 19

Conclusions Single Top is still elusive on its way to be observed at the TeVatron, though. Single Top will be an interesting process to study at LHC, both in the beginning (low luminosity phase) and later Lots of work is ongoing both at the Tevatron and LHC will surely benefit from the experience. 20

TeVatron current results (III) Combined Channels likelihood 695 pb -1 (s+t) Upper Limit σ < 4.3 pb @ 95% C.L. 21