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Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/ILDWelcome.pdf20 Sep 2007: CaliceLCFILC-ABDPhenomenology. UK ILD involvement needs to build on this strengthIn immediate future “unlikely” to get new fundingDifficult to start genuinely new activities. -
Microsoft PowerPoint - ILDUK
https://www.hep.phy.cam.ac.uk/~thomson/talks/ILDUK.pdf28 Sep 2007: CaliceLCFILC-ABDPhenomenology. UK ILD involvement needs to build on this strengthIn immediate future (LoI) “unlikely” to get much new fundingDifficult to start genuinely new activities. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/EPS2007_Thomson.pdf18 Jul 2007: a new approach to calorimetry. EPS HEPP-2007, Manchester, July 20th Mark Thomson 7. ... Tracking calorimeter” – requiresa new approach to ECAL/HCALreconstruction. ILC calorimetric performance = HARDWARE SOFTWARE. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/GLD_LDC_thomson.pdf29 May 2007: aim to learn something new…- very fresh. Use simplified LDC cost model as starting pointSystem Fractional Cost Proportional toECAL 0.29 Active area. -
PowerPoint Presentation
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/Sonja.ppt21 Sep 2007: to extend and improve performance, e.g. by exploring new algorithms. In both these areas. ... Vertexing:. aim to improve run-time performance by interfacing new vertex fitter to the code. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/Pandora_Paris2007.pdf3 May 2007: ILC software mtg., Paris 3/5/2007 Mark Thomson 24. Angular Dependence (NEW). ... v) Iterative Reclustering. Iterative Reclustering Strategies. vi) Photon Recovery (new in v01-01). -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_qed.pdf30 Jul 2007: the two new particles). e-. e+. µ-. µ+. γ. 1q2. e e. -
Slide 1
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/CMB-GLDC-Cambs07.ppt21 Sep 2007: Target layer thickness 0.1%X0 (100mm Si). Thin sensors. New support materials. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_ew.pdf31 Jul 2007: W Wb. t. Mtop2. H. W. ln(mH)? • BUT measured mass also sensitive to new particlesvia “loop corrections”. • ... Questions/Problems with the Standard Model. Our understanding of particle physics is still evolving.Over the next few years many new -
The ILD (LDC) Detector ConceptThe ILD (LDC) Detector ConceptTies ...
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/ILD.pdf21 Sep 2007: Auto-calibratingbut non-linear. New era for scintillator–based detectors:. High granularity at relatively low cost. ... Lots of data accumulated, analyses are very preliminaryExpect many new and interesting results in the near future. -
Fran k G aede , LD C U K ...
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/gaede_ldc_framework.pdf21 Sep 2007: 007. 2. Outlineoverview core toolsLCIO, Mokka, Marlin, Gear, (LCCD) status and new featuresinstallation, build tools. ... MarlinGUI, flow charts new logging mechanism:. streamlog_out( DEBUG ) << “ digitizing hit : “ << hit->getCellID() << std::endl ; -
CALICE-UK and ILD
https://www.hep.phy.cam.ac.uk/~thomson/meetings/ild/talks/watson_ILD_1.ppt21 Sep 2007: again needs new effort (I just don’t have time). Perspective:. What Next. ... Optimisation of new code. Slow procedure… takes about 6 CPU-days per variation. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_intro.pdf30 Jul 2007: The discussion is important some of the ideas will bevery new to you … there are no foolish questions! ... I3. Particles appear in groups of equal mass. Suggestive of sub-structure – QUARKSmany of these new particles were just different -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/IoP2007_Thomson_ILC.pdf3 Apr 2007: new particle thresholds. ILC PHYSICS PROGRAMME. Can accumulate large samples ofcleanly identified/well-measured events. ... Limited by typical HCAL resolution of > 50%/E(GeV). a new approach to calorimetry. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_weak.pdf31 Jul 2007: 4. 5. β decay and neutrinosIn 1930 Pauli proposed that a new unobserved particle, “the neutrino”was emitted with the e- in β decay. -
Particle Flow Calorimetry and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/RALFinal.pdf10 Apr 2007: Limited by typical HCAL resolution of > 50%/E(GeV). a new approach to calorimetry. ... New paradigm – nobody really knows how to approach this. So where are we now? -
Particle Flow Calorimetry at the ILCM. A. Thomson Cavendish ...
https://www.hep.phy.cam.ac.uk/~thomson/publications/hsw06.pdf16 Jan 2007: In this manner hits are added to clustersor are used to seed new clusters. ... Associations maybe made with hits in the previous 3 layers. If no association is made, the hit is used toseed a new cluster. -
Neutrino Oscillations and the MINOS experiment
https://www.hep.phy.cam.ac.uk/~thomson/lectures/iss/iss2007_qcd_quarks.pdf30 Jul 2007: the string some ofthe energy is converted into mass – new qq pairs are created. -
Observation of Muon Neutrino Disappearance with the MINOS Detectorsin …
https://www.hep.phy.cam.ac.uk/~thomson/publications/PhysRevLett_97_191801.pdf14 Apr 2007: 4Brookhaven National Laboratory, Upton, New York 11973, USA5Lauritsen Laboratory, California Institute of Technology, Pasadena, California 91125, USA. ... 10Physics Department, Columbia University, New York, New York 10027, USA. PRL 97, 191801 (2006) P H -
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH OPAL PR 42420th July ...
https://www.hep.phy.cam.ac.uk/~thomson/publications/pr424.pdf25 Jul 2007: This characteristic event topology is ofinterest both for measuring aspects of W physics and for exploring the potential productionof new particles leading to the same experimental signature. ... The WW νν event selec-tion described here first requires
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