Report from the ILD Meeting Ties Behnke ILC project meeting 26.9.2014.

Slides:



Advertisements
Similar presentations
ILD Meeting Oshu City Introduction and Charge Ties Behnke, Yasuhiro Sugimoto for the ILD JSB Oshu City 2014 D L I.
Advertisements

ILD Resource Survey 2014/9/9 Y. Sugimoto 1. Committee under MEXT ILC Task Force in MEXT Academic experts committee Particle-Nuclear physics WG Members.
Manpower and space requirements for ILD 2015/1/13 Y. meeting at SLAC 1.
Beyond the ALCPG David B. MacFarlane Associate Laboratory Director for PPA.
Snowmass 25 AugustMark Thomson 1 PFA Progress and Priorities Mark Thomson (for Steve Magill, Felix Sefkow, Mark Thomson and Graham Wilson)  Progress at.
Ties Behnke, Vasiliy Morgunov 1SLAC simulation workshop, May 2003 Pflow in SNARK: the next steps Ties Behnke, SLAC and DESY; Vassilly Morgunov, DESY and.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Pair backgrounds for different crossing angles Machine-Detector Interface at the ILC SLAC 6th January 2005 Karsten Büßer.
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.
1 Benchmarking the SiD Tim Barklow SLAC Sep 27, 2005.
The Physics Potential of the PHENIX VTX and FVTX Detectors Eric J. Mannel WWND 13-Apr-2012.
Status of ILC Barry Barish Caltech / GDE 17-Aug-07.
 k0k0 ++ -- -- p ILC Technical Design Report Physics and Detectors – Detailed Baseline Design Juan A. Fuster Verdú, IFIC-Valencia PAC Meeting, KEK.
ILD meeting Welcome/Introduction 2015/4/23 Y. 1.
HEPAP and P5 Report DIET Federation Roundtable JSPS, Washington, DC; April 29, 2015 Andrew J. Lankford HEPAP Chair University of California, Irvine.
Discussion/ Planning Session -ILD organisation: status and plans -Concrete plans -Report from the R&D group: Jan Strube -Report from the parameter group:
MEXT Review Process in Japan 2014/7/16 Y. Sugimoto 1.
1 The ILD LoI IDAG Referees for ILD Benchmarking – J.A. Hewett, W.G. Li Tracking – R. Nickerson Calorimetry – D. Green MDI – T. Himmel.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
F R&D on Monolithic and Vertically Integrated Pixel Detectors Special Focus Meeting Marcel Demarteau LCWS08 November 17, 2008 Chicago.
Precise Measurements of SM Higgs at the ILC Simulation and Analysis V.Saveliev, Obninsk State University, Russia /DESY, Hamburg ECFA Study Workshop, Valencia.
Z AND W PHYSICS AT CEPC Haijun Yang, Hengne Li, Qiang Li, Jun Guo, Manqi Ruan, Yusheng Wu, Zhijun Liang 1.
Karsten Büßer Beam Induced Backgrounds at TESLA for Different Mask Geometries with and w/o a 2*10 mrad Crossing Angle LCWS 2004 Paris April 19 th 2004.
SiD R&D on PFA and Calorimetry -> IDAG guidance. -> Present PFA situation. -> Developing a timeline for PFA development. -> Calorimetry aspects.
Preparing for the SiD LoI SiD Parallel Session TILC08 March 5, 2008 John Jaros.
Vienna Fast Simulation LDT Munich, Germany, 17 March 2008 M. Regler, M. Valentan Demonstration and optimization studies by the Vienna Fast Simulation Tool.
ILD Optimization Why – when – what Ties Behnke, DESY Henri Videau, LLR.
Karsten Büßer Instrumentation of the Forward Region of the TESLA Detector International Europhysics Conference on High Energy Physics Aachen, July 19th.
Status Report on ILC Project in Japan Seiichi SHIMASAKI Director, Office for Particle and Nuclear Research Promotion June 19, 2015.
CLICdp achievements in 2014 and goals for 2015 Lucie Linssen, CERN on behalf of the CLICdp collaboration CLIC workshop, January 30 th
Taikan Suehara, Belgrade, 7 Oct page 1 Hybrid ECAL: optimization and related developments Taikan Suehara H. Hirai, H. Sumida, Y. Sudo, T.
Top quark IIHE Future interests  Towards data taking → new software  Have a broader physics output  Link theory-experiment  Calibration and.
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
“Huge” Detector Concept 3 Sep 2004 ECFA LC Durham Satoru Yamashita ICEPP, University of Tokyo On behalf of many colleagues Towards our common.
Lukens - 1 Fermilab Seminar – July, 2011 Observation of the  b 0 Patrick T. Lukens Fermilab for the CDF Collaboration July 2011.
Ties Behnke: Event Reconstruction 1Arlington LC workshop, Jan 9-11, 2003 Event Reconstruction Event Reconstruction in the BRAHMS simulation framework:
(Some thoughts/reminders on) Calibration/alignment scenarios for ILD/ILC Jan Timmermans – NIKHEF Amsterdam 07 Sep 2014ILD meeting Oshu1.
LCWS11 – Tracking Performance at CLIC_ILD/SiD Michael Hauschild - CERN, 27-Sep-2011, page 1 Tracking Performance in CLIC_ILD and CLIC_SiD e + e –  H +
Detector Cooperation with CLIC PAC Pohang meeting November 3, 2009 F. Richard LAL/Orsay 11/03/20091.
Assembly scenario of ILD Si trackers 2015/4/21 Yasuhiro 1.
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.
RECFA September Kenneth Österberg, University of Helsinki Experimental e + e - physics – LEP&LC DELPHI Major finnish LEP contribution analysis.
ILD meeting Thursday May 30, 2013 Ties Behnke, Yasuhiro Sugimoto.
SiD Vertexing and Tracking Contribution to the LOI Bill Cooper Marcel Demarteau Ron Lipton Rich Partridge Dong Su For the SiD Vertex/Tracking Group SiD.
Mark Thomson University of Cambridge High Granularity Particle Flow Calorimetry.
12 March 2006, LCWS06, BangaloreS. Bhattacharya 1 Satyaki Bhattacharya The Standard Model Higgs Search at the LHC University of Delhi.
Palaiseau, 13/1/ 2005 P. Colas - Optimising tracking 1 Optimising a Detector from the Tracking Point-of-View P.Colas, CEA Saclay constraints role Optimisation.
DØ Beauty Physics in Run II Rick Jesik Imperial College BEACH 2002 V International Conference on Hyperons, Charm and Beauty Hadrons Vancouver, BC, June.
Argonne’s Rôle in ZEUS José Repond Argonne National Laboratory DOE Visit, Germantown, March 11 th, 2004.
Higgs Summary Alexei Raspereza On behalf of Higgs Working Group ECFA Workshop, Warsaw 12/06/2006 Outline  Current Status  Contributions in Warsaw  Theory.
Octobre 2007LAL Orsay Very Forward Instrumentation of the ILC Detector Wolfgang Lohmann, DESY.
DETECTOR RESEARCH AND DEVELOPMENT Fred Borcherding 1.
FNAL Users’ Meeting– June Fermilab Users’ Meeting CMS Physics from Early LHC Running Dan Green Fermilab For the CMS Collaboration.
LCC Physics and Detector Report
Relations with concept groups
Electroweak Physics Towards the CDR
Electroweak physics at CEPC
Electroweak Physics Towards the CDR
ILD Technical Coordination
Particle detection and reconstruction at the LHC (IV)
Strategy Ties Behnke
Introduction to the Workshop
Electroweak Physics Towards the CDR
Sub-Detector Assembly Area Summary of discussion at ALCW2015
ILD Optimisation: towards 2012 University of Cambridge
STAR Geometry and Detectors
Snowmass on the Mississippi
Yasuhiro Okada, Executive Director, KEK
SUSY SEARCHES WITH ATLAS
Presentation transcript:

Report from the ILD Meeting Ties Behnke ILC project meeting

OSHU Strong local support ILD / ILC rather visible in the city

UNESCO Heritage site: very close by

Close to the IP: Project by local high school students

ILD meeting 85 registered participants from 32 institutes

Participants

Goals Re-invent ILD “the detector” Put ILD up against the physics agenda of the ILC: how are we doing? Are we doing the right things? Are we doing things right? Re-invent ILD “the organisation” Make the physics case through realistic physics studies

Reinvent ILD: Organisation Signup Procedure for ILD: 57 groups so far have signed the memorandum of participation by ILD Institute assembly has been met the first time Election for chair of the institute assembly is ongoing. Discussion on new structure for ILD will be driven by the institute assembly.

Reinvent ILD: Detector

External Review of ILD

Demarteau: Key Statements.. a strength of ILD is that it is BIG... A weakness of the ILD is the use of a TPC...although the SIT is reasonably well motivated the need for SET and ETD has not been demonstrated... On the very positive side ILD has been fairly aggressive in designing a most comprehensive ILD detector that is very performant.. On the negative side, the detector resorts to the use of multiple technologies to overcome the shortcomings of main technologies... The collaboration has very effectively used the R&D collaborations in their design efforts and performance studies.. The collaboration would profit from clear technology decisions over the next couple of years

1. Demonstrate ILD Capabilities & Choices Quantify requirements for light Higgsino benchmark based on FullSim: – Particle ID from DE/dx & calorimeter – Low p t tracking in pair background -> VTX timing Jet / vertex charge for A FB (top) Systematics for at least one ultra-precise channel, eg H->bb, M W or top couplings: – formulate as requirements on JES, p-scale, etc

2. Justify our basic choices Why a TPC? – Expect several arguments out of studies on previous slide: dE/dx, low momentum tracks, … Physics driven requirements on – Momentum & impact parameter resolutions – Photon energy & angle resolution – JER – dE/dx ? – Low mometum reach

Tracking ILD has a composite system -TPC central tracker -Silicon outside and inside -O(10um) resolution for Silicon system Contribution of SET to the overall tracking performance. SET justification 1: Improvement of the momentum resolution

Tracking Major issue: Field distortions in the TPC. -From local E-field effects -From global B-field effects Calibration of possible using internal consistency But SET justification 2: External point will help a lot (needed precision? )

Size optimization Impact of ECAL radius on particle flow performance: Seems to be fairly flat.

Granularity optimization Dependence is stronger at higher energies Behaviour at very small cell sizes: not understood. (Software artefact?)

Tau reconstruction Particle flow is not all: -What about tau reconstruction/ other exclusive states? -No conclusion yet, though initial studies suggest no strong dependence.

Changing the ILD size Changing ILD: Requires careful re-optimzation also of the hardware Non trivial task if you want to move away from simple naïve scaling models. Changing ILD: Requires careful re-optimzation also of the hardware Non trivial task if you want to move away from simple naïve scaling models.

Forward Direction Rather detailed design of the forward direction exists Fairly complete engineering has been done L* change request Discussion on crossing angle Re-optimization of the forward region would require a serious simulation effort to understand the impact on reducing L*. ILD position: we need to study this, but are very sceptical to go below 4m

Calibration Scenarios Z-peak running: – Are the canonical numbers based on LEP experience (10 pb -1 commissioning, pb -1 quick re-alignment) sufficient for ILD detector modularity? – Simulation alignment excercise needed? Alternatives at nominal beam energy? – Z return – Momentum calibration from Z, J/ψ, Υ (e.g. Graham Wilson at AWLC14) Cosmics, yes (LHC has shown importance), but: – 0.5% duty cycle due to power pulsing – reduced rate, because of underground location, but maybe not so deep B-field mapping – Can we measure it precisely enough? (study on use of detailed map in reconstruction ongoing) 07 Sep 2014ILD meeting Oshu23

Physics at the ILC Physics case for the ILC has been made, But We need to get better! Be more realistic, in particular, fold in running scenarios. Be broader, show, where ILC really would make a difference.

Higgs Physics Dominated by tracking resolution: Challenge to the trackers? Higgs recoil is a strong point for 250 GeV running, BUT Utilize hadronic Higgs decays: 350 GeV as good? All other channels are better at 350+ GeV (WW Fusion contributes)

BSM Physics A strong focus has been on Higgs Physics We need to have a broader focus, and show the impact ILC will have on the overall physics landscape: Physics beyond the Standard Model Impact of ILC on Heavy Higgs searches:

Where to go? “Technical” performance does not vary strongly with radius. Particle flow and tracking seem ok. What about other parameters? Need to translate into proper physics performance Need to study more than just particle flow Need to understand behaviour at higher energies Need to also look at impact on detector integration etc. Next step: Define a number of benchmark reactions Define a (small) number of ILD models to study

Committee under MEXT ILC Task Force in MEXT Academic experts committee Particle-Nuclear physics WG Members are physicists from; HEP(6), Nuclear physics, Cosmic-ray, Astronomy, Accelerator(2), Particle theory, Nuclear theory, Cosmology, Science communication TDR validation WG Members are accelerator physicists from; KEK(3), JAERI, Riken(2), NIRS, HiSOR, JASRI/Spring8, CROSS-Tokai /shingi/chousa/shinkou/038/ind ex.htm We need information from detector groups 28

Resource survey in ILD Timeline – Time line was drawn based on the schedule in TDR (Figure in Vol.3-II) and recent CFS study – Assembly hall is assumed to be built in 2 years from ground breaking – Duration of “Assembly on site” can be modified by sub-system groups 29

Status of the survey 30 Total FTE neededFTE on site Annual budget

Conclusion ILD is alive and well Significant interest and support Active community does studies Re-optimization of ILD is ongoing Serious physics studies using ILD are ongoing Not covered: Clear R&D plans exist for the major systems Next meeting: at LCWS 2014 and Spring 2015 Asian workshop Dedicated ILD workshop Summer 2015 in Europe