ATLAS Upgrade Program Sarah Demers, US ATLAS Fellow with BNL

Slides:



Advertisements
Similar presentations
Ken Bell – Rutherford Appleton Laboratory
Advertisements

Freiburg Seminar, Sept Sascha Caron Finding the Higgs or something else ideas to improve the discovery ideas to improve the discovery potential at.
Higgs Searches using Vector Boson Fusion. 2 Why a “Low Mass” Higgs (1) M H
Fourth Generation Leptons Linda Carpenter UC Irvine Dec 2010.
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
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.
1 Hadronic In-Situ Calibration of the ATLAS Detector N. Davidson The University of Melbourne.
1 Search for Excited Leptons with the CMS Detector at the Large Hadron Collider. Andy Yen, Yong Yang, Marat Gataullin, Vladimir Litvine California Institute.
February 19th 2009AlbaNova Instrumentation Seminar1 Christian Bohm Instrumentation Physics, SU Upgrading the ATLAS detector Overview Motivation The current.
The SLHC and the Challenges of the CMS Upgrade William Ferguson First year seminar March 2 nd
Nick Hadley Run II Physics (I) Nick Hadley The University of Maryland New Perspectives 2000 Fermilab - June 28, 2000.
Jet Studies at CMS and ATLAS 1 Konstantinos Kousouris Fermilab Moriond QCD and High Energy Interactions Wednesday, 18 March 2009 (on behalf of the CMS.
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.
Measurement of the branching ratios for Standard Model Higgs decays into muon pairs and into Z boson pairs at 1.4 TeV CLIC Gordana Milutinovic-Dumbelovic,
FIMCMS, 26 May, 2008 S. Lehti HIP Charged Higgs Project Preparative Analysis for Background Measurements with Data R.Kinnunen, M. Kortelainen, S. Lehti,
Electroweak and Related Physics at CDF Tim Nelson Fermilab on behalf of the CDF Collaboration DIS 2003 St. Petersburg April 2003.
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.
Higgs Reach Through VBF with ATLAS Bruce Mellado University of Wisconsin-Madison Recontres de Moriond 2004 QCD and High Energy Hadronic Interactions.
ATLAS B-Physics Reach M.Smizanska, Lancaster University, UK
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
Bangalore, India1 Performance of GLD Detector Bangalore March 9 th -13 th, 2006 T.Yoshioka (ICEPP) on behalf of the.
INCLUSIVE STANDARD MODEL HIGGS SEARCHES HIGGS SEARCHES WITH ATLAS Francesco Polci LAL Orsay On behalf of the ATLAS collaboration. SUSY08 – Seoul (Korea)
Study of pair-produced doubly charged Higgs bosons with a four muon final state at the CMS detector (CMS NOTE 2006/081, Authors : T.Rommerskirchen and.
Alternatives: Beyond SUSY Searches in CMS Dimitri Bourilkov University of Florida For the CMS Collaboration SUSY06, June 2006, Irvine, CA, USA.
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
A/H  and A/H  decays at the LHC Outline of the talk: The LHC and ATLAS,CMS MSSM A/H Higgs production A/H  A/H  Conclusions HEP2003 Europhysics.
RECENT RESULTS FROM THE TEVATRON AND LHC Suyong Choi Korea University.
Hiroshima Higgs Workshop 2006, Jan. 17 – 19, 2006 Higgs Searches at the Tevatron Kazuhiro Yamamoto (Osaka City University) for the CDF Collaboration 1.Tevatron.
From the Standard Model to Discoveries - Physics with the CMS Experiment at the Dawn of the LHC Era Dimitri Bourilkov University of Florida CMS Collaboration.
Particle Physics II Chris Parkes Top Quark Discovery Decay Higgs Searches Indirect mW and mt Direct LEP & LHC searches 2 nd Handout.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
La Thuile, March, 15 th, 2003 f Makoto Tomoto ( FNAL ) Prospects for Higgs Searches at DØ Makoto Tomoto Fermi National Accelerator Laboratory (For the.
Trilepton+top signal from chargino-neutralino decays of MSSM charged Higgs bosons 17 June 2004, 9 th Nordic LHC Physics Workshop, Copenhagen Christian.
Studies of the Higgs Boson at the Tevatron Koji Sato On Behalf of CDF and D0 Collaborations 25th Rencontres de Blois Chateau Royal de Blois, May 29, 2013.
Low Mass Standard Model Higgs Boson Searches at the Tevatron Andrew Mehta Physics at LHC, Split, Croatia, September 29th 2008 On behalf of the CDF and.
Fourth Generation Leptons Linda Carpenter April 2011.
SESAPS November 11, B. Scurlock, University of Florida1 Bobby Scurlock Darin Acosta Paolo Bartalini Richard Cavanaugh Alexey Drozdetskiy Guenakh.
Joshua Moss (Ohio State University) on behalf of the ATLAS Collaboration ICHEP 2012, Melbourne 6 July 2012 ATLAS Electroweak measurements of W and Z properties.
XLIX International Winter Meeting on Nuclear Physics January 2011 Bormio, Italy G. Cattani, on behalf of the ATLAS Collaboration Measurement of.
Searches for Additional Higgs Bosons in Extensions of the Standard Model at ATLAS Ashutosh Kotwal Duke University for the ATLAS Collaboration 19 th International.
Determining the CP Properties of a Light Higgs Boson
IOP HEPP Conference Upgrading the CMS Tracker for SLHC Mark Pesaresi Imperial College, London.
Multilepton production at HERA
Particle detection and reconstruction at the LHC (IV)
Stop->4 bodies signal samples with 2 leptons in final state
Venkat Kaushik, Jae Yu University of Texas at Arlington
Central Exclusive Production of BSM Higgs bosons decaying to jets
The ATLAS Experiment at the LHC
Small Extra Dimension Graviton Detection at ATLAS
ATLAS Collaboration 3000 Physicists including 1000 students.
SUSY post LHC-8: what’s excluded, what’s not
The Silicon Track Trigger (STT) at DØ
by M. Della Negra, P. Jenni, and T. S. Virdee
Louisiana Tech University
Plans for checking hadronic energy
Jessica Leonard Oct. 23, 2006 Physics 835
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
Strong Electroweak Symmetry Breaking from
Searches at LHC for Physics Beyond the Standard Model
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
New Approaches to Hadronic Final State Reconstruction
Search for Narrow Resonance Decaying to Muon Pairs in 2.3 fb-1
SUSY SEARCHES WITH ATLAS
Study of the LFV channel t  3m
Experimental and theoretical Group Torino + Moscow
Measurement of the Single Top Production Cross Section at CDF
Susan Burke, University of Arizona
Search for a New Vector Resonance in the pp WWtt+X Channel at LHC
Presentation transcript:

ATLAS Upgrade Program Sarah Demers, US ATLAS Fellow with BNL Yale University 2013 US LHC Users Organization Annual Meeting

What ATLAS vulnerabilities appear with increased luminosity and time?

detector detector in pile-up What ATLAS vulnerabilities appear with increased luminosity and time? detector detector in pile-up

PHYSICS

PHYSICS The Standard Model Open access to new ideas and searches Continue to test SM Continue to use SM physics to measure efficiencies Open access to new ideas and searches Increase flexibility of trigger system

Current Work Includes: Insertable B-Layer Topological Trigger Combining muon and calorimeter objects – can make requirements on angular distributions masses to select signal or reject BG

Fast TracKer (FTK) Electronics for global tracking on every L1 Trigger to provide early access to tracking information at Level 2. Main motivation: b- and t-tagging

FTK Efficiencies for muons and pions with respect to truth (simulation) and offline reconstruction ATLAS-TDR-021-2013

2018 – 2022 300 fb-1 60 - 80 pile-up events Phase-I

Phase-I Level1 Calorimeter Trigger/Readout Muon New Small Wheel

Level 1 Calorimeter Trigger: Increased Granularity

Level 1 Calorimeter Trigger: Increased Granularity Current L1 Trigger Tower

Level 1 Calorimeter Trigger: Increased Granularity Current L1 Trigger Tower Full Detector Granularity

Level 1 Calorimeter Trigger: Increased Granularity Current L1 Trigger Tower Phase-II Supercell Full Detector Granularity

Muon New Small Wheel (NSW) A set of precision tracking and trigger detectors that can work at high rates with excellent time and spatial resolution. ATLAS-TDR-020-2013

Muon New Small Wheel Low purity (currenty) in the end-cap region

Segment finding for a 2 TeV Z’ decaying Muon New Small Wheel Segment finding for a 2 TeV Z’ decaying to a pair of muons

Phase-II 2024 – 203x 3000 fb-1 140 – 200 pile-up events Level 1 Track Trigger

The ATLAS Tracking Chambers

an example upgrade layout

channel occupancy with 200 pile-up interactions

Constraints Include Access

From ATLAS Phase-II Letter of Intent

Motivation for the Track Trigger

Performance assumptions based on full simulation for an upgraded ATLAS detector at a High-Luminosity LHC The ATLAS Collaboration ATLAS-PUB-2013-009

25 GeV for electrons and muons 60 GeV for photons and taus Performance assumptions based on full simulation for an upgraded ATLAS detector at a High-Luminosity LHC The ATLAS Collaboration ATLAS-PUB-2013-009 offline cuts of 25 GeV for electrons and muons 60 GeV for photons and taus 180 GeV for Missing ET

Performance assumptions based on full simulation for an upgraded ATLAS detector at a High-Luminosity LHC The ATLAS Collaboration ATLAS-PUB-2013-009

https://twiki.cern.ch/twiki/bin/view/AtlasPublic/UpgradePhysicsStudies

Sensitivity of ATLAS at HL-LHC to flavour changing neutral currents in top quark decays t → cH, with H → gg ATLAS-PHYS-PUB-2013-012

Prospects for benchmark SSUY search at high luminosity with the ATLAS Detector ATL-PUB-2013-001 The 95 % CL exclusion limits (dashed) and 5-sigma discovery reach (solid) for 300 inverse fb (red) and 3000 fb-1 (black) in the stop, neutralino-1 mass plane assuming a stop to top and neutralino-1 decay with a branching ratio of 100 %.

Propoer Decay Time Resolution

Conclusions Physics Goals drive the ATLAS upgrade Plan Increased Performance and Flexibility of our detector and trigger will allow us to use SM physics to understand our detector in new machine environments continue to Probe the Higgs Boson search for other physics beyond the SM respond to what we uncover at high energy!