MAP MDI at SLAC. Thomas Markiewicz, SLAC Muon Collider Higgs Factory Workshop, UCLA March 22, 2013
|
|
- Patrick Barker
- 5 years ago
- Views:
Transcription
1 MAP MDI at SLAC Thomas Markiewicz, SLAC Muon Collider Higgs Factory Workshop, UCLA March 22, 2013
2 Muon Accelerator Program (MAP) MDI In 2013 SLAC submitted an MDI-focused work package to MAP mgmt. for funding Scope: Concentrate on the Higgs Factory (1 st ) and 3 TeV collider (2 nd ) Develop a realistic implementation of a detector with IR magnets and local shielding Characterize performance To better understand and control the background source terms, a small group of mostly volunteers has: Acquired the current (preliminary) HF lattice Begun to study the lattice with rapid tracking tools: (Decay)Turtle, DIMAD & Transport - Uli Wienands & Lew Keller Created a FLUKA model of the lattice to understand front end issues of significance to the detector: Takashi Maruyama - Energy deposition in local masking, etc. Communicate regularly with MAP MDI & Physics/Detector groups Not yet begun Look at files of background in an SiD inspired detector in the LCSIM environment - Norman Graf et al 2
3 Introduction to Muon Colliders: First Principles Input: Neuffer s talk at MAP 2012 Winter meeting at SLAC Lattice: Alexahin (preliminary) v8.2 Muon lifetime = 1300 revolutions in 300m ring at 62.5 GeV Fill = 1000 turns= 1msec Fill frequency =15 Hz, 1 bunch/beam, 2E12 muons/bunch At injection 20 kjoules/beam, 300 kw/beam Decay electrons: Peak decay rate = 5.1E6/m/beam Average electron energy in lab = 22 GeV Average electron angle in lab w.r.to muon = 1.7 mrad Peak e- power lost to ring = 5.4 MW/beam Average e- power lost to ring = 56.4 kw/beam Average e- power density =188 W/m/beam 3
4 Decay Electron Kinematics Elab (GeV) Theta_lab (rad.) Elab (GeV) Theta_lab (rad.) 4
5 Muon Collider Geometry in FLUKA Takashi Maruyama Alexahin s MAD deck Use MAD survey file Wrote a program to read the survey file and generate FLUKA input. Primitive geometry definitions Region definitions Material definitions Magnetic field type (bends, quads, sexts) and strength Collider parameters are arbitrarily chosen, but can be changed easily. Tunnel radius (2 m) Tunnel wall thickness (50 cm) Magnet shape and size (Bend: 2 m x 1 m) Beampipe thickness (1 mm) Beampipe radius (10 cm) Concrete Steel Air Dirt 5
6 Study #1 Backgrounds crossing scoring plane at 5m from source points Scoring plane Tunnel filling concrete shield added - decays 6
7 An example: Decays at z=22.7m without tunnel filling concrete shield 7
8 Particle flux reaching the IR Particles / 5 million decays e- e+ photon neutron muon pion Distance from IP (m) 8
9 Decays at s = 6.4 m e+/e- Neutrons Tunnel Y (cm) X (cm) X (cm) 9
10 Decays at s = 22.7 m Neutrons Muons Y (cm) - + X (cm) X (cm) 10
11 General Comments on background type & location e+/e- and Inside beam pipe and magnet bore Neutrons Magnet bore More diffuse over tunnel Muons Bend magnets sweep muons and Magnet body acts like a shield ~50 muons/meter Hadrons Smaller flux and easier to shield 11
12 Study 2: IP Conic Mask Study Vary thickness at tip and look at particles penetrating the mask Quad Masks & Final Focus Combined Function Quad M1_Cone M1_Barrel M2_Cone QLB1 200 QLB r=22cm r=23cm QLB2 QLB Inspired by Mokhov 1.5 TeV design Use large apertures specified in Alexahin lattice for IP magnets Maintain 6cm long beampipe at IP Scale beampipe radius to 4cm radius based on 13.5cm to 1.78 cm radii of apertures of first quad in 1.5 TeV versus HF lattices 12
13 IR Mask Varied the thickness at tip from 5-75mm Count particles decays between 0 and 4 m. 5E6 decays/m rate x 4m => results absolutely normalized Sig_x = Sig_y = 5cm at 1 st quad 3 Tesla Solenoid 13
14 Particle flux leaving beampipe and mask vs. Mask thickness e+/e-/1000/cm 0.5 cm 1.5 cm 3.5 cm 7.5 cm e+/e- Photons/1000/cm 14
15 Particle flux vs. Mask thickness 0.5 cm 1.5 cm 3.5 cm 7.5 cm Neutrons Neutrons/cm 15
16 Comments Need a HF reference design with agreed to parameters: Emittances, beam sizes, etc. Beam pipe radii, apertures, VXD length, Designs too immature to invest vast computing resources (and time) Rapid prototyping tools & investigation of parameter space preferable We at SLAC look forward to continuing this work if MAP decides it is worth it 16
Preliminary Design of m + m - Higgs Factory Machine-Detector Interface
Fermilab Accelerator Physics Center Preliminary Design of m + m - Higgs Factory Machine-Detector Interface Nikolai Mokhov Y. Alexahin, V. Kashikhin, S. Striganov, I. Tropin, A. Zlobin Fermilab Higgs Factory
More informationHiggs Factory Magnet Protection and Machine-Detector Interface
Higgs Factory Magnet Protection and Machine-Detector Interface Nikolai Mokhov Fermilab MAP Spring Workshop May 27-31, 2014 Outline MDI Efforts Building Higgs Factory Collider, Detector and MDI Unified
More informationMDI and detector modeling
MDI and detector modeling Nikolai Terentiev (Carnegie Mellon U./Fermilab) On behalf of N. Mokhov, S. Striganov (Fermilab), C. Gatto, A. Mazzacane, V. Di Benedetto (INFN/Fermilab/INFN Lecce and Università
More informationBeam loss background and collimator design in CEPC double ring scheme
Beam loss background and collimator design in CEPC double ring scheme Sha Bai 9 th International Particle Accelerator Conference (IPAC 18), Vancouver, Canada, Apr 29-May 4, 2018. 2018-05-01 Outline Introduction
More information1.1 Machine-Detector Interface
FERMILAB-PUB-11-535-APC 1 1.1 Machine-Detector Interface 1.1.1 Introduction Nikolai V. Mokhov, Fermilab, Batavia, IL, USA Mail to: mokhov@fnal.gov In order to realize the high physics potential of a Muon
More informationColliders and the Machine Detector Interface
Colliders and the Machine Detector Interface M. Sullivan SLAC National Accelerator Laboratory for the Hong Kong University of Science and Technology Jockey Club Institute for Advanced Study High Energy
More informationLCWS 05 Machine Detector Interface Design Updates. Tom Markiewicz SLAC 22 March 2005
LCWS 05 Machine Detector Interface Design Updates SLAC 22 March 2005 ILC WG4 Strawman Layout of BDS with 20 mrad and 2 mrad IRs logically complete P P P E E P E E 2/ 20 Warm LC Collimation System Design
More information1.5 TeV Muon Collider background rejection in ILCroot Si VXD and Tracker (summary report)
1.5 TeV Muon Collider background rejection in ILCroot Si VXD and Tracker (summary report) N. Terentiev* (Carnegie Mellon U./Fermilab) V. Di Benedetto, C. Gatto (INFN) A. Mazzacane, N. Mokhov, S. Striganov
More informationLER Beam-Beam Collimation. Studies Using TURTLE
LER Beam-Beam Collimation Studies Using TURTLE Stephanie Majewski, Witold Kozanecki October 21, 2004 Abstract We report the results of a TURTLE study designed to explore the use of collimation to minimize
More informationLattice Design and Performance for PEP-X Light Source
Lattice Design and Performance for PEP-X Light Source Yuri Nosochkov SLAC National Accelerator Laboratory With contributions by M-H. Wang, Y. Cai, X. Huang, K. Bane 48th ICFA Advanced Beam Dynamics Workshop
More informationIPBI-TN June 30, 2004
Spray Electron Beam for Tests of Linear Collider Forward Calorimeter Detectors in SLAC End Station A R. Arnold UMass Amherst, Amherst MA 01003 T. Fieguth Stanford Linear Accelerator Center Menlo Park,
More informationMachine Detector Interface at Electron Colliders. Hongbo Zhu (IHEP, Beijing)
Machine Detector Interface at Electron Colliders Hongbo Zhu (IHEP, Beijing) Outline Introduction Interaction Regions Single ring, pretzel scheme, head-on collision Radiation Backgrounds Final Focusing
More informationSC magnets for Future HEHIHB Colliders
SC magnets for Future HEHIHB Colliders presented by L. Bottura WAMS, Archamps, March 22-23,2004 Overview Few selected examples of drivers for R&D in the next 10 years LHC upgrades scenarios (why? how?)
More informationPoS(NuFact2017)088. EMuS in CSNS. Guang Zhao 1. Institute of High Energy Physics Beijing, China
1 Institute of High Energy Physics Beijing, China E-mail: zhaog@ihep.ac.cn In this presentation, we report the recent progress in EMuS at CSNS. The following topics will be discussed: a) the base design
More informationSuperconducting Magnets for Future Electron-Ion Collider. Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA
Superconducting Magnets for Future Electron-Ion Collider Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA Mini-workshop on Accelerator, IAS, HKUST, Hong Kong, January 18-19, 2018 1 Outline
More informationCase study: Energy deposition in superconducting magnets in IR7
Case study: Energy deposition in superconducting magnets in IR7 AMT Workshop A.Ferrari, M.Magistris, M.Santana, V.Vlachoudis CERN Fri 4/3/2005 Overview Motivation Geometry and Simulation setup Studies:
More informationSimulation of the ILC Collimation System using BDSIM, MARS15 and STRUCT
Simulation of the ILC Collimation System using BDSIM, MARS5 and STRUCT J. Carter, I. Agapov, G. A. Blair, L. Deacon, A. I. Drozhdin, N. V. Mokhov, Y. Nosochkov, A. Seryi August, 006 Abstract The simulation
More information2.24 Simulation Study of K L Beam: K L Rates and Background Ilya Larin Department of Physics Old Dominion University Norfolk, VA 23529, U.S.A.
2.24 Simulation Study of K L Beam: K L Rates and Background Ilya Larin Department of Physics Old Dominion University Norfolk, VA 23529, U.S.A. Abstract We report our simulation results for K L -beam and
More informationSBF Accelerator Principles
SBF Accelerator Principles John Seeman SLAC Frascati Workshop November 11, 2005 Topics The Collision Point Design constraints going backwards Design constraints going forward Parameter relations Luminosity
More informationDetector and Physics studies for a 1.5TeV Muon Collider Experiment
Detector and Physics studies for a 1.5TeV Muon Collider Experiment *, C. Gatto (INFN) A. Mazzacane, N. Mokhov, S. Striganov (Fermilab) N. Terentiev (Carnegie Mellon U./Fermilab) MAP 2014 Winter Collaboration
More informationThe High-Power-Target System of a Muon Collider or Neutrino Factory
The High-Power-Target System of a Muon Collider or Neutrino Factory K. McDonald Princeton U. (August 29, 2014) NuFact 14 U Glasgow KT McDonald NuFact 14 (U Glasgow) August 29, 2014 1 The Target System
More informationSLAC-PUB Submitted to Radiation Protection and Dosimetry. Work supported by Department of Energy contract DE-AC02-76SF00515
SLAC-PUB-11088 CALCULATIONS OF NEUTRON AND PHOTON SOURCE TERMS AND ATTENUATION PROFILES FOR THE GENERIC DESIGN OF THE SPEAR3 STORAGE RING SHIELD S. H. Rokni, H. Khater, J. C. Liu, S. Mao and H. Vincke
More informationTeV Scale Muon RLA Complex Large Emittance MC Scenario
TeV Scale Muon RLA Complex Large Emittance MC Scenario Alex Bogacz and Kevin Beard Muon Collider Design Workshop, BNL, December 1-3, 29 Outline Large Emittance MC Neuffer s Collider Acceleration Scheme
More informationCEPC Detector and Physics Studies
CEPC Detector and Physics Studies Hongbo Zhu (IHEP) On Behalf of the CEPC-SppC Study Group FCC Week 2015, 23-27 March, Washington DC Outline Project overview Higgs Physics @ CEPC The CEPC detector Machine-Detector
More informationRESEARCH AND DEVELOPMENT OF FUTURE MUON COLLIDER*
FERMMILAB-CONF-12-213-APC RESEARCH AND DEVELOPMENT OF FUTURE MUON COLLIDER* K. Yonehara #, Fermilab, Batavia, IL 60510, USA Abstract Muon collider is a considerable candidate of the nextgeneration high-energy
More informationIR and backgrounds of ILC and Super KEKB. Hitoshi Yamamoto
IR and backgrounds of ILC and Super KEKB Hitoshi Yamamoto ILC configuration 500 GeV CM 14mrad crossing angle 3000 bunches/train, 1ms/train 5 trains/sec IR design of typical ILC detector (SiD, GLD, LDC,
More informationMuon Front-End without Cooling
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Muon Front-End without Cooling CERN-Nufact-Note-59 K. Hanke Abstract In this note a muon front-end without cooling is presented. The muons are captured, rotated
More informationCollider Rings and IR Design for MEIC
Collider Rings and IR Design for MEIC Alex Bogacz for MEIC Collaboration Center for Advanced Studies of Accelerators EIC Collaboration Meeting The Catholic University of America Washington, DC, July 29-31,
More informationYear- 1 (Heavy- Ion) Physics with CMS at the LHC
Year- 1 (Heavy- Ion) Physics with CMS at the LHC Edwin Norbeck and Yasar Onel (for the CMS collaboration) University of Iowa For the 26 th Winter Workshop on Nuclear Dynamics Ocho Rios, Jamaica 8 January
More informationReconstruction in Collider Experiments (Part IX)
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments (Part IX) Peter Loch University of Arizona Tucson,
More informationMachine-Detector Interface for the CEPC
Machine-Detector Interface for the CEPC Hongbo ZHU (IHEP) Joint effort of the Detector and Accelerator Groups Machine-Detector Interface Machine Detector Interface (MDI) covers all aspects that are common
More informationAccelerator development
Future Colliders Stewart T. Boogert John Adams Institute at Royal Holloway Office : Wilson Building (RHUL) W251 Email : sboogert@pp.rhul.ac.uk Telephone : 01784 414062 Lectures aims High energy physics
More informationJLEIC forward detector design and performance
Jefferson Lab E-mail: ryoshida@jlab.org A major part of the physics program at the Electron-Ion Collider being planned in the US is the exploration of nucleon and nuclear structure. This program means
More informationSiD concept adapted to CLIC
SiD and CLIC Outline: Adaptation of SiD detector for CLIC Use of SiD software for CLIC Tracking studies Calorimetry studies Engineering of CLIC_SiD General layout Forward region layout with QD0 integration
More informationStudy and Simulation of the Radiation background of the ATLAS Experiment at CERN using the Monte Carlo method
Study and Simulation of the Radiation background of the ATLAS Experiment at CERN using the Monte Carlo method Maria Lymperaiou ECE NTUA Under the supervision of Professor Evangelos Gazis March 30, 2018
More informationImproved final doublet designs for the ILC baseline small crossing angle scheme
Improved final doublet designs for the ILC baseline small crossing angle scheme R. Appleby, P. Bambade August 1, 2006 Abstract The ILC baseline consists of two interaction regions, one with a 20mrad crossing
More informationVery low Emittance Muon Beam using positron beam on target
References: Very low Emittance Muon Beam using positron beam on target M. Antonelli (INFN-LNF) Chicago (USA), ICHEP 2016 M.Antonelli, E.Bagli, M.Biagini, M.Boscolo, G.Cavoto, P.Raimondi and A.Variola,
More informationUCLA Ring Cooler Simulation
MUCOOL/MICE Cooling Theory Meeting Feb. 5 2002 UCLA Ring Cooler Simulation Yasuo Fukui UCLA e-mail: fukui@slac.stanford.edu March 7-8 2002 UCLAWorkshop The Use of Ring Cooler for a Neutrino Factory and
More informationModern Accelerators for High Energy Physics
Modern Accelerators for High Energy Physics 1. Types of collider beams 2. The Tevatron 3. HERA electron proton collider 4. The physics from colliders 5. Large Hadron Collider 6. Electron Colliders A.V.
More informationOverview of HEMC Scheme
Overview of HEMC Scheme R. B. Palmer, (BNL) JLab 2/28/2011 My birthday Progress on Cooling simulations New Acceleration sequence with higher transmission New System transmission estimate New Wall power
More informationBeam Dump Experiments at JLab and SLAC
Beam Dump Experiments at JLab and SLAC Brief History (E137 at SLAC) BDX at Jefferson Lab Detector and signal Backgrounds Expected Sensitivity Elton S. Smith, Jefferson Lab On behalf of the BDX Collaboration
More informationEDMS No: Revision: Pages: Date: Addendum to IT-3036/EP/CMS
EDMS No: Revision: Pages: Date: CMS-IZ-CI-0003 draft Page 1 of 45 15.11.02 EDMS No: Revision: Pages: Date: 396215 1.1 6 09.09.2003 Addendum to IT-3036/EP/CMS Technical Specification for Supply and Installation
More informationCLIC Detector studies status + plans
CLIC Detector studies status + plans Contents: - Introduction to CLIC accelerator - 2004 CLIC Study group report: "Physics at the CLIC Multi-TeV Linear Collider - CERN participation in Linear Collider
More informationCERN R&D on Linear Collider Detectors. Lucie Linssen CERN
CERN R&D on Linear Collider Detectors Lucie Linssen CERN 1 Outline Outline: Introduction CLIC physics Detector issues Comparison between ILC and CLIC Linear Collider Detector R&D plans Outlook 2 Introduction
More informationGeneral Considerations
Advantages of Muons Advantages of leptons over hadrons Energetic Interaction simplicity Minimal synchrotron radiation at high energies Can bend: not forced to linac like e Reuse accelerating structures
More informationCOMPRESSED SUSY AND BEAMCAL SIMULATION STUDIES AT SCIPP
SCIPP ILC SID/FCAL SIMULATION GROUP JANE SHTALENKOVA BRUCE SCHUMM, WILLIAM WYATT, BENJAMIN SMITHERS COMPRESSED SUSY AND BEAMCAL SIMULATION STUDIES AT SCIPP ILC BEAMCAL Accepts E+&E- scattered between 5
More informationSPPC Study and R&D Planning. Jingyu Tang for the SPPC study group IAS Program for High Energy Physics January 18-21, 2016, HKUST
SPPC Study and R&D Planning Jingyu Tang for the SPPC study group IAS Program for High Energy Physics January 18-21, 2016, HKUST Main topics Pre-conceptual design study Studies on key technical issues R&D
More informationForward Region, Energy Spectrometer, Polarimeter. Snowmass Klaus Mönig
Forward Region, Energy Spectrometer, Polarimeter Klaus Mönig Snowmass 2005 1 Klaus Mönig MDI questions related to this talk 9) Is a 2 mrad crossing angle sufficiently small that it does not significantly
More informationUpstream Polarimetry with 4-Magnet Chicane
2005 International Linear Collider Workshop Stanford, U.S.A. Upstream Polarimetry with 4-Magnet Chicane N. Meyners, V. Gharibyan, K.P. Schüler DESY, Hamburg, Germany We have extended an earlier polarimeter
More informationFirst propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division
First propositions of a lattice for the future upgrade of SOLEIL A. Nadji On behalf of the Accelerators and Engineering Division 1 SOLEIL : A 3 rd generation synchrotron light source 29 beamlines operational
More informationInteraction Region Designs for Electron Colliders
Interaction Region Designs for Electron Colliders M. Sullivan SLAC National Accelerator Laboratory 1 A Brief History of e+e- Colliders and Backgrounds The very first e+e- collider was AdA made here at
More informationLHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva
LHC Detectors and their Physics Potential Nick Ellis PH Department, CERN, Geneva 1 Part 1 Introduction to the LHC Detector Requirements & Design Concepts 2 What is the Large Hadron Collider? Circular proton-proton
More informationFuture prospects for the measurement of direct photons at the LHC
Future prospects for the measurement of direct photons at the LHC David Joffe on behalf of the and CMS Collaborations Southern Methodist University Department of Physics, 75275 Dallas, Texas, USA DOI:
More information6 Bunch Compressor and Transfer to Main Linac
II-159 6 Bunch Compressor and Transfer to Main Linac 6.1 Introduction The equilibrium bunch length in the damping ring (DR) is 6 mm, too long by an order of magnitude for optimum collider performance (σ
More informationBeam losses versus BLM locations at the LHC
Geneva, 12 April 25 LHC Machine Protection Review Beam losses versus BLM locations at the LHC R. Assmann, S. Redaelli, G. Robert-Demolaize AB - ABP Acknowledgements: B. Dehning Motivation - Are the proposed
More informationNEXT GENERATION B-FACTORIES
NEXT GENERATION B-FACTORIES M. Masuzawa, KEK, Tsukuba, Japan Abstract The KEKB and PEP-II B factories have achieved world record luminosities while doubling or tripling their original design luminosities.
More informationPhysics 736. Experimental Methods in Nuclear-, Particle-, and Astrophysics. - Accelerator Techniques: Introduction and History -
Physics 736 Experimental Methods in Nuclear-, Particle-, and Astrophysics - Accelerator Techniques: Introduction and History - Karsten Heeger heeger@wisc.edu Homework #8 Karsten Heeger, Univ. of Wisconsin
More informationAccelerators. Lecture V. Oliver Brüning. school/lecture5
Accelerators Lecture V Oliver Brüning AB/ABP http://bruening.home.cern.ch/bruening/summer school/lecture5 V) LEP, LHC + more LEP LHC Other HEP Projects Future Projects What else? LEP Precision Experiment:
More informationIntroduction to the Standard Model
Introduction to the Standard Model Bill Murray, RAL, Quarks and leptons Bosons and forces The Higgs March 2002 1 Outline: An introduction to particle physics What is the Higgs Boson? Some unanswered questions
More informationMESON AREA 1000 GeV STUDY. C. N. Brown, A. L. Read, A. A. Wehmann Fermi National Accelerator Laboratory
-375 MESON AREA 1000 GeV STUDY C. N. Brown, A. L. Read, A. A. Wehmann Fermi National Accelerator Laboratory This report attempts to collect together preliminary thoughts on how protons from the Energy
More informationVHEeP: A very high energy electron proton collider based on protondriven plasma wakefield acceleration
VHEeP: A very high energy electron proton collider based on protondriven plasma wakefield acceleration Allen Caldwell (MPI) Matthew Wing (UCL/DESY/Univ. Hamburg) Introduction Accelerator based on plasma
More informationCMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS NOTE 1996/005 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Performance of the Silicon Detectors for the
More informationGG6 summary. Valery Telnov Snowmass, Aug.19, 2005,
GG6 summary Valery Telnov Snowmass, Aug.19, 2005, Goal of the Global Group GG6 GG6, Options: Understand requirements and configurational issues related to possible alternatives to e+e- collisions, including
More informationASPECTS OF MACHINE INDUCED BACKGROUND IN THE LHC EXPERIMENTS
ASPECTS OF MACHINE INDUCED BACKGROUND IN THE LHC EXPERIMENTS Abstract G.Corti and V.Talanov Λ, CERN, Geneva, Switzerland In our report we review different aspects of the LHC Machine Induced Background
More informationThe Tiny Muon versus the Standard Model. Paul Debevec Physics 403 November 14 th, 2017
The Tiny Muon versus the Standard Model Paul Debevec Physics 403 November 14 th, 2017 BNL E821 Muon g-2 Collaboration Standard Model of Particle Physics Components of the Standard Model of Particle Physics
More informationThe MERIT High-Power Target Experiment
The MERIT High-Power Target Experiment 3 rd High-Power Target Workshop Bad Zurzach, Switzerland September 11, 2007 Brookhaven National Laboratory The Neutrino Factory Target Concept Maximize Pion/Muon
More informationThe LHC. Part 1. Corsi di Dottorato Corso di Fisica delle Alte Energie Maggio 2014 Per Grafstrom CERN and University of Bologna
The LHC Part 1 Corsi di Dottorato Corso di Fisica delle Alte Energie Maggio 2014 Per Grafstrom CERN and University of Bologna Organizzazione Part 1 Part 2 Part 3 Introduction Energy challenge Luminosity
More informationCMS Event Simulation
CMS Event Simulation Nicole A. Larsen Department of Physics, Georgia Institute of Technology, Atlanta, GA, 33 (Dated: August 11, 6) The CMS Detector located at the Large Hadron Collider at CERN recently
More informationFragments in eic. S.White 6/5/10 Forward physics at colliders. measurement of fragments Experience from RHIC/LHC the machine
Fragments in eic S.White 6/5/10 Forward physics at colliders http://arxiv4.library.cornell.edu/abs/1003.4252 http://indico.cern.ch/conferencedisplay.py?confid=94115 measurement of fragments Experience
More informationTools of Particle Physics I Accelerators
Tools of Particle Physics I Accelerators W.S. Graves July, 2011 MIT W.S. Graves July, 2011 1.Introduction to Accelerator Physics 2.Three Big Machines Large Hadron Collider (LHC) International Linear Collider
More informationSubcritical Fission Reactor and Neutrino Factory Based on Linear Collider
2005 International Linear Collider Workshop - Stanford, U.S.A. Subcritical Fission Reactor and Neutrino Factory Based on Linear Collider I. F. Ginzburg Sobolev Institute of Mathematics and Novosibirsk
More informationTheory English (Official)
Q3-1 Large Hadron Collider (10 points) Please read the general instructions in the separate envelope before you start this problem. In this task, the physics of the particle accelerator LHC (Large Hadron
More informationAnalyzing CMS events
Quarknet University of Rochester, March 23, 2012 Analyzing CMS events Questions in Particle Physics Introducing the Standard Model The Large Hadron Collider The CMS detector W and Z bosons: decays ispy
More informationParticles and Universe: Particle accelerators
Particles and Universe: Particle accelerators Maria Krawczyk, Aleksander Filip Żarnecki March 24, 2015 M.Krawczyk, A.F.Żarnecki Particles and Universe 4 March 24, 2015 1 / 37 Lecture 4 1 Introduction 2
More informationStatus of Optics Design
17th B2GM, February 5, 2014 Status of Optics Design Y. Ohnishi /KEK 17th B2GM KEK, February 5, 2014 Contents! Lattice parameters! Dynamic aperture under influence of beam-beam effect! Lattice preparation
More informationMagnet Modelling and its Various Uses at SLAC
Magnet Modelling and its Various Uses at SLAC Informal presentation by Cherrill Spencer, SLAC s Magnet Engineer, to the Mini- Workshop on Magnet Simulations for Particle Accelerators at PAC05. 18th May
More informationG4beamline A beam/particle simulation program based on Geant4. Muons, Inc. Innovation in research
G4beamline A beam/particle simulation program based on Geant4. Muons, Inc. Innovation in research G4beamline goals G4beamline is intended to perform simulations as realistically as possible. With validation
More informationTracker material study with the energy flow through the CMS electromagnetic calorimeter. Riccardo Paramatti, Ambra Provenza
Tracker material study with the energy flow through the CMS electromagnetic calorimeter Riccardo Paramatti, Ambra Provenza The electromagnetc calorimeter (ECAL) To detect photons and electrons iη=85 iη=1
More information(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.
Introduction One of the main events in the field of particle physics at the beginning of the next century will be the construction of the Large Hadron Collider (LHC). This machine will be installed into
More informationA brief history of accelerators, detectors and experiments: (See Chapter 14 and Appendix H in Rolnick.)
Physics 557 Lecture 7 A brief history of accelerators, detectors and experiments: (See Chapter 14 and Appendix H in Rolnick.) First came the study of the debris from cosmic rays (the God-given particle
More informationThe Detector Design of the Jefferson Lab EIC
The Detector Design of the Jefferson Lab EIC Jefferson Lab E-mail: mdiefent@jlab.org The Electron-Ion Collider (EIC) is envisioned as the next-generation U.S. facility to study quarks and gluons in strongly
More informationSimulation Studies for a Polarimeter at the International Linear Collider (ILC)
Project Report Summer Student Program 2007 Deutsches Elektronen-Synchrotron (DESY) Hamburg, Germany Simulation Studies for a Polarimeter at the International Linear Collider (ILC) Moritz Beckmann Leibniz
More informationLHC. Jim Bensinger Brandeis University New England Particle Physics Student Retreat August 26, 2004
Experiments @ LHC Jim Bensinger Brandeis University New England Particle Physics Student Retreat August 26, 2004 Outline of Presentation Existing Spectrometers A Certain Sameness The Basic Interaction
More informationLinear Collider Collaboration Tech Notes. Design Studies of Positron Collection for the NLC
LCC-7 August 21 Linear Collider Collaboration Tech Notes Design Studies of Positron Collection for the NLC Yuri K. Batygin, Ninod K. Bharadwaj, David C. Schultz,John C. Sheppard Stanford Linear Accelerator
More informationNote. Performance limitations of circular colliders: head-on collisions
2014-08-28 m.koratzinos@cern.ch Note Performance limitations of circular colliders: head-on collisions M. Koratzinos University of Geneva, Switzerland Keywords: luminosity, circular, collider, optimization,
More informationBeam-induced radiation in the compact muon solenoid tracker at the Large Hadron Collider
PRAMANA c Indian Academy of Sciences Vol. 74, No. 5 journal of May 2010 physics pp. 719 729 Beam-induced radiation in the compact muon solenoid tracker at the Large Hadron Collider A P SINGH 1,, P C BHAT
More informationThe Particle World. This talk: What is our Universe made of? Where does it come from? Why does it behave the way it does?
The Particle World What is our Universe made of? Where does it come from? Why does it behave the way it does? Particle physics tries to answer these questions. This talk: particles as we understand them
More informationLecture 2 & 3. Particles going through matter. Collider Detectors. PDG chapter 27 Kleinknecht chapters: PDG chapter 28 Kleinknecht chapters:
Lecture 2 & 3 Particles going through matter PDG chapter 27 Kleinknecht chapters: 1.2.1 for charged particles 1.2.2 for photons 1.2.3 bremsstrahlung for electrons Collider Detectors PDG chapter 28 Kleinknecht
More informationThe Electron-Ion Collider
The Electron-Ion Collider C. Tschalaer 1. Introduction In the past year, the idea of a polarized electron-proton (e-p) or electron-ion (e-a) collider of high luminosity (10 33 cm -2 s -1 or more) and c.m.
More informationBulk shielding design for the MAX IV facility
Bulk shielding design for the MAX IV facility Magnus Lundin 1, Lennart Isaksson 1, Bent Schröder 1 1 Lund University, MAX-lab, P.O. Box 118, SE-221 Lund, Sweden Abstract This paper reports on the design
More informationHigh Energy Physics. QuarkNet summer workshop June 24-28, 2013
High Energy Physics QuarkNet summer workshop June 24-28, 2013 1 The Birth of Particle Physics In 1896, Thompson showed that electrons were particles, not a fluid. In 1905, Einstein argued that photons
More informationThe Large Hadron electron Collider at CERN
The Large Hadron electron Collider at CERN A. Polini (for the LHeC Collaboration) Outline: Introduction Accelerator, Interaction Region and Detector Physics Highlights Future and Outlook A. Polini LHeC
More informationOverview of Acceleration
Overview of Acceleration R B Palmer, Scott Berg, Steve Kahn (presented by Steve Kahn) Nufact-04 RF Frequency Acc types and System Studies Linacs RLA s FFAG s Injection/Extraction US Study 2a acceleration
More informationThe 2015 erhic Ring-Ring Design. Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory
The 2015 erhic Ring-Ring Design Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory The Relativistic Heavy Ion Collider RHIC Two superconducting storage rings 3833.845 m circumference
More informationThe Very Large Hadron Collider Beam Collimation System
The Very Large Hadron Collider Beam Collimation System A.I. Drozhdin, N.V. Mokhov, A.A. Sery, Fermilab, P.O. Box 5, Batavia, IL 65 USA INTRODUCTIONS Even in good operational conditions, a finite fraction
More informationRadiation damage in diamond sensors at the CMS experiment of the LHC
Radiation damage in diamond sensors at the CMS experiment of the LHC Moritz Guthoff on behalf of the CMS beam monitoring group ADAMAS Workshop 2012, GSI, Germany IEKP-KIT / CERN KIT University of the State
More informationAnalyses with photons or electrons with early LHC data at the CMS experiment
Analyses with photons or electrons with early LHC data at the CMS experiment Dottorando: Daniele Franci Relatori: Prof. Egidio Longo Dott. Daniele del Re Prof. Shahram Rahatlou Seminario progetto di tesi,
More informationGeant4 Physics Lists: Status and Proposed Upgrades. Dennis Wright (SLAC) 25 February 2011
Geant4 Physics Lists: Status and Proposed Upgrades Dennis Wright (SLAC) 25 February 2011 Outline Contents of a few preferred Geant4 physics lists Updating/augmenting the physics lists Comparing Fluka and
More informationRecent results at the -meson region from the CMD-3 detector at the VEPP-2000 collider
Recent results at the -meson region from the CMD-3 detector at the VEPP-2000 collider Vyacheslav Ivanov *1, Evgeny Solodov 1, Evgeny Kozyrev 1, and Georgiy Razuvaev 1 1 Budker Institute of Nuclear Physics,
More informationFull-Acceptance Detector Integration at MEIC
Full-Acceptance Detector Integration at MEIC Vasiliy Morozov for MEIC Study Group Electron Ion Collider Users Meeting, Stony Brook University June 27, 2014 Lattice design of geometrically-matched collider
More information