Mechanical Engineering

Size: px
Start display at page:

Download "Mechanical Engineering"

Transcription

1 Mechanical Engineering The Mechanical Engineering within STFC Technology is project based, projects varying in time from a few days to many years. The larger projects are usually collaborations with other research institutes e.g. CERN (the European Particle Physics Centre), and the hardware may be built anywhere in the world. Our Engineering includes; Mechanical Engineering Design concepts, development of ideas Project Management financial management, Health & Safety, use of resources Project Engineering - planning, milestones, costings Structural Analysis Use of FEA, analysing designs, vibration, seismic calculations Procurement contractual requirements, delivery details Assembly Supervision, training, auditing Particular experience in Beamline Engineering, with associated Vacuum technology and motion control. Typical projects are International and are collaborative requiring both technical leadership and team member skills

2 STFC Technology Project areas detailed on following pages ATLAS (A Toroidal Lhc ApparatuS) CMS (Compact Muon Solenoid) LHCb (Large Hadron Collider beauty) SR (Synchrotron Radiation) Instruments Beamline components Magnet testing Advanced LIGO (Laser Interferometric Gravitational wave Observatory) MICE (Muon Ionisation Cooling Expt) T2K 4m Superconducting Helical Undulator

3 ATLAS (A Toroidal Lhc ApparatuS) Silicon Trackers (SCT) The SCT trackers lie in the centre of the ATLAS experiment. They determine the properties of the charged particles produced by the colliding beams. Demanding Mechanical Requirements: Stiff and extremely stable structures to accurately position the detectors and support power, cooling, and readout services. These must be constructed from non-magnetic materials and be radiation tolerant to withstand 10yrs+ of operation. The absolute minimum amount of material must be used since it will absorb particles and make the data less accurate.

4 STFC work areas on ATLAS 1) SCT Wheels 2) End Cap Main Structure 3) Environmental Housing 4) SCT Services 5) SCT Tooling 6) Services Arm Links to further information on ATLAS An early prototype cylinder

5 1 SCT Wheels A set of 9 structural disks covered with silicon detector modules and services, there are termed Wheels.

6 2 SCT Structure A stable structure to support the Wheels. A carbon fibre reinforced plastic (CFRP) sandwich structure was chosen to give a lightweight, very stable structure. Positional stability better than a few 10s of m over a day required. Design analysed to ensure strong and stiff enough for 200kg load. Load tests on completed structure proved capability Analysis showed that deflections due to any likely vibrational input would be very small and not affect data.

7 3 Functions: 3 SCT Environmental Housing a) Enable the tracker to be a thermally neutral sealed containment for N2 dry gas purge with grounding & shielding requirements. b) Plastic foams, low emissivity surfaces and external heaters produce a partially active thermal enclosure to minimising insulating volume. c) Heat loads from the external environment and internal electrical services were balanced internally to ensure the assembly was thermally neutral.

8 4 SCT Services Routing of services (optical fibre, electrical, fluid cooling, gas purge) This included defining the length of each of the services. This routing shaped many of the other major parts (Internal patch panels, support structure, environmental housing). This required specialised cable trays, hardware & wrappings for thermal management / Grounding & Shielding, and the compact multi-service patch panels.

9 Required to 1) Assemble the detector 5 ATLAS SCT Tooling 2) integrate it into ATLAS

10 6 Services Arm The superconducting ATLAS end cap and barrel toroid magnets require copious quantities of cyrogens and other services. These services required an 18 metre long flexible support arm which was not commercially available.

11 CMS (Compact Muon Solenoid) CMS is also a particle measuring instrument on the LHC. The requirement here was to provide a mechanical support structure for the large mass of 7500 detector crystals, yet allow them to be extremely precisely positioned. This was achieved with D shaped backplates which are cantilevered from the main body of CMS by a large aluminium support ring. This ring had to be specially cast. The back plates have hundreds of holes carefully machined in them (see picture) to allow the accurate location of the detectors. The design allows the services to be routed back through the backplate and support ring. Following pictures Backplate and Support Ring:machining and attachment Perspective view from pit Accurately positioning the detectors Links to further information on CMS: Wikipedia CMS Public domain CMS Outreach

12 CMS

13 CMS

14 Accurately positioning the detectors CMS

15 LHCb Experi ment Photo shows CERN (European Particle Physics Research Centre) near Geneva and the path of the large underground accelerator

16 LHCb Experiment RICH1 RICH2 Key components are the RICH (Ring Imaging Cherenkov) detectors. The largest of these is RICH2 which measures the velocity of charged particles. In combination with the momentum this permits their identification.

17 RICH1Detector STFC responsibility VELO Seal STFC responsibility: Composite Exit Window & Beam Pipe Seal

18 RICH2 CF4 gas volume : ~100 m³

19 FEA of RICH2 Superstructure Distortions due to gravity < 1mm in 10m

20 RICH2 in Final Position Magnet RICH2 RICH1 E Cal

21 Multi Polarimeter SR (Synchrotron Radiation) Instruments The Multilayer Polarimeter is a collaborative project between STFC and Diamond Light Source Ltd (DLS) Working Principle This is based on the polarising properties of reflecting surfaces and transmitting thin films referred to as multilayers. The polarimeter will be a mobile instrument and will be connected to existing beamlines in the region between 90 and 1200eV. Incident light will pass into a UHV vessel and through the retarding multilayer to introduce phase retardation before being reflected by the analyser multilayer. The intensity of the reflected light will be measured by a suitably positioned detector. The instrument comprises of other associated optical elements mounted on an optical bench within a vacuum vessel and uses pinholes to define the beam axis and includes a beam filtering system. The instrument is mounted on a Hexapod support and manipulation system. Following pages give more details on: Hexapod Rotation of Multilayers Multilayer Exchange System

22 Hexapod The Hexapod, supplied by Oxford Danfysik, has 6 degrees of motorised motion and is supported and driven by 6 high precision actuators. The linear actuators are driven by stepper motors and gearboxes with linear encoders giving positional feedback and include end of travel limit switches. The Hexapod is controlled using EPICS software with a Delta-Tau based motion control system. The user software is capable of orientating the instrument supported from the upper plinth around any pre-determined co-ordinate system or point in space with positional feedback.

23 Rotation of Multilayers The retarder and analyser multilayers each require two axes of rotation and the detector also has one rotation axis. The five axes of rotation are provided using in-vacuum Huber goniometers with Renishaw encoders providing an angular resolution of as small as A motor driven linear stage positioned onto the analyser stage will be used with graded multilayers.

24 Multilayer Exchange System The multilayers are prone to degradation and to allow continuous operation of the polarimeter at different beamline energies, a magazine-type arrangement will be required to store the multilayers within the instrument. Individual multilayers will be mounted in their own dedicated frame holders, transfer arms and a manual rack driven transporter will be used to facilitate transfer of frame holders between the magazine and their working positions in both the retarder and analyser positions

25 Beamline Components STFC have 50 years experience of designing and manufacturing beamline components, whether for a proton synchrotron such as ISIS, or a light source e.g SRS and DIAMOND. This includes the range of magnets, accelerating cavities, monochromators, undulators/wigglers, sample positioning devices, and spatial detector systems that are required. Fundamental engineering of adjustable magnet stands, support systems and alignment tooling are vital to produce a good working beamline. Following pages: Example pictures of High Specification beamline components

26 Beamline Components 1

27 Beamline Components 2

28 Magnet Testing STFC have extensive experience in testing different magnet types e.g. quadrupoles, undulators etc.

29 LIGO The STFC team has played a major role in the Advanced LIGO (Laser Interferometric Gravitational wave Observatory) which is being assembled in the USA. Development: STFC developed the suspension concept from a physics model and previous prototypes built in the US. We optimised the structure to achieve a high enough stiffness and developed the mass designs to make the whole system easy to assemble and cost effective to manufacture. Manufacture We have manufactured and built the Noise Prototype and the final articles are in production.

30 LIGO CAD Model Real Framework

31 LIGO QUAD Assembly

32 MICE (Muon Ionisation Cooling Expt) MICE is an essential step in accelerator R&D towards the realisation of a neutrino factory, which is the physicists next generation tool for probing matter; and could prove decisive in understanding the matter-antimatter asymmetry of the universe. MICE is a Technology Demonstrator to prove the vital cooling mechanism -It requires a large new dedicated facility with a precursor Muon beam line into which the novel cooling channel is assembled This facility is being built by STFC at RAL Major STFC Responsibilities Project Management, together with support from international committee of collaborators Co-ordination and integration of beamline components from abroad Creation of the facility and all the infrastructure Provision of key components e.g. Liquid Hydrogen system, Superconducting Pion decay channel Running of the experiment in conjunction with ISIS, our proton accelerator More info on following pages: Model of cooling channel Infrastructure Hall layout Photos Links for further information

33 MICE 3D Model of proposed cooling channel 3 Absorber Focus Coil Modules Tracker Module 4 RF Cavities/module

34 MICE Infrastructure The MICE facility requires construction of major infrastructure to support the muon beamline and cooling channel e.g. ; A Hall with power, lighting, ventilation, lifting equipment Massive 200 tonne magnetic shielding walls Provision of flat stable support for 20+ tonne beamline items Biological shielding Liquid Hydrogen handling plant High Voltage equipment Chilled water plant RF Amplifiers Magnet power supplies This infrastructure is near completion

35 Layout of MICE Hall

36 MICE Photos of Early construction/integration work on the facility and components

37 T2K The T2K experiment is a second generation long-baseline neutrinooscillation experiment to study nature of neutrinos. Artificial neutrino beam generated in the JHF 50GeV high-intensity proton accelerator in JAERI (Tokai, Ibaraki) is shoot toward the 50kton water Cherenkov detector, Super-Kamiomande, which is located about 1000m underground in Kamioka mine(gifu) and is 295km away from Tokai. STFC areas of work Target and Remote Handling Management (Info on following 2 pages) Near detector (the ND280) Baffle and the Beamline Remote Seals

38 T2K TARGET components TITANIUM GRAPHITE Ø46mm ~960mm Ø226mm

39 T2K Remote Handling Design work

40 Superconducting Helical Undulator An exciting development programme has been carried out to produce a highly accurate and very long 4m helical undulator. The HeLiCal collaboration consisting of Technology, ASTeC, the German institute DESY and the universities of Liverpool and Durham have designed and manufactured the prototype magnet as part of research work for linear colliders. The following photographs show the mechanical construction of the former/cables, and the final 4m long module.

41 Superconducting Helical Undulator The ribbon is required to run in the grooves in continuous layers with no gap between the layers. The picture below shows a sectioned undulator prototype. The former is a two-start helical spring with a tube inserted in the bore. The picture below shows a short length prototype.

42 Superconducting Helical Undulator Machining the long former was very challenging. Firstly a steel cylinder was gun drilled to get the accurate centre bore. This was subsequently turned concentric to the bore using an optical alignment technique and then the two helixes were progressively milled using a special technique developed in our workshop. The essential copper tube down the centre is added afterwards. A technique of unusually winding the superconducting filaments as a flat ribbon has been perfected, before finally the former is potted and machined to accurate dimensions. The picture shows the 1.8m former being machined, with four supporting stays along its length

43 Superconducting Helical Undulator The development team with the completed 4 metre long undulator

44 Update: Success! The undulator magnets have now been powered up to 280 Amps with no quenching and left running for a period. The helium cryogen is only being boiled off very slowly, and a constant vacuum is being maintained. This represents an excellent success for the project.

Layout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC

Layout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC Layout and prototyping of the new ATLAS Inner Tracker for the High Luminosity LHC Ankush Mitra, University of Warwick, UK on behalf of the ATLAS ITk Collaboration PSD11 : The 11th International Conference

More information

MuCool Test Area Experimental Program Summary

MuCool Test Area Experimental Program Summary MuCool Test Area Experimental Program Summary Alexey Kochemirovskiy The University of Chicago/Fermilab Alexey Kochemirovskiy NuFact'16 (Quy Nhon, August 21-27, 2016) Outline Introduction Motivation MTA

More information

The ATLAS Toroid Magnet

The ATLAS Toroid Magnet The ATLAS Toroid Magnet SUN Zhihong CEA Saclay DAPNIA/SIS 1 The ATLAS Magnet System The ATLAS Barrel Toroid Mechanical computations on the Barrel Toroid structure Manufacturing and assembly of the Barrel

More information

3 General layout of the XFEL Facility

3 General layout of the XFEL Facility 3 General layout of the XFEL Facility 3.1 Introduction The present chapter provides an overview of the whole European X-Ray Free-Electron Laser (XFEL) Facility layout, enumerating its main components and

More information

The Compact Muon Solenoid Experiment at the LHC. Images of Assembly and Installation

The Compact Muon Solenoid Experiment at the LHC. Images of Assembly and Installation The Compact Muon Solenoid Experiment at the LHC Images of Assembly and Installation Contents 1. Civil Engineering Pages 8 to 13 2. Assembly in the Surface Building Pages 14 to 35 3. Lowering of the Heavy

More information

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction THE LEP PROJECT - STATUS REPORT Herwig Schopper CERN 1211 Geneva 23, Switzerland Introduction LEP is an e + e - collider ring designed and optimized for 2 100 GeV. In an initial phase an energy of 2 55

More information

Nano Beam Position Monitor

Nano Beam Position Monitor Introduction Transparent X-ray beam monitoring and imaging is a new enabling technology that will become the gold standard tool for beam characterisation at synchrotron radiation facilities. It allows

More information

CEBAF Overview June 4, 2010

CEBAF Overview June 4, 2010 CEBAF Overview June 4, 2010 Yan Wang Deputy Group Leader of the Operations Group Outline CEBAF Timeline Machine Overview Injector Linear Accelerators Recirculation Arcs Extraction Systems Beam Specifications

More information

THE CRYOGENIC SYSTEM OF TESLA

THE CRYOGENIC SYSTEM OF TESLA THE CRYOGENIC SYSTEM OF TESLA S. Wolff, DESY, Notkestr. 85, 22607 Hamburg, Germany for the TESLA collaboration Abstract TESLA, a 33 km long 500 GeV centre-of-mass energy superconducting linear collider

More information

Grounding for EMC at the European XFEL

Grounding for EMC at the European XFEL Grounding for EMC at the European XFEL Herbert Kapitza, Hans-Jörg Eckoldt, Markus Faesing Deutsches Elektronensynchrotron (DESY) D-22603 Hamburg, Germany Email: herbert.kapitza@desy.de Abstract The European

More information

Philippe Lebrun & Laurent Tavian, CERN

Philippe Lebrun & Laurent Tavian, CERN 7-11 July 2014 ICEC25 /ICMC 2014 Conference University of Twente, The Netherlands Philippe Lebrun & Laurent Tavian, CERN Ph. Lebrun & L. Tavian, ICEC25 Page 1 Contents Introduction: the European Strategy

More information

Status of ATLAS & CMS Experiments

Status of ATLAS & CMS Experiments Status of ATLAS & CMS Experiments Atlas S.C. Magnet system Large Air-Core Toroids for µ Tracking 2Tesla Solenoid for inner Tracking (7*2.5m) ECAL & HCAL outside Solenoid Solenoid integrated in ECAL Barrel

More information

HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION

HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION K.V. Zolotarev *, A.M. Batrakov, S.V. Khruschev, G.N. Kulipanov, V.H. Lev, N.A. Mezentsev, E.G. Miginsky, V.A. Shkaruba,

More information

Technology Transfer at CERN

Technology Transfer at CERN Technology Transfer at CERN Enrico Chesta Head of CERN Technology Transfer and Intellectual Property Management Section Knowledge Transfer Group, FP Department How can CERN have an impact beyond fundamental

More information

SPECIFICATIONS FOR A 4.7 TESLA/310MM BORE ACTIVELY SHIELDED MAGNET SYSTEM

SPECIFICATIONS FOR A 4.7 TESLA/310MM BORE ACTIVELY SHIELDED MAGNET SYSTEM SPECIFICATIONS FOR A 4.7 TESLA/310MM BORE ACTIVELY SHIELDED MAGNET SYSTEM Prepared by:- Magnex Scientific Limited The Magnet Technology Centre 6 Mead Road Oxford Industrial Park Yarnton, Oxford OX5 1QU,

More information

Preparing for the Future: Upgrades of the CMS Pixel Detector

Preparing for the Future: Upgrades of the CMS Pixel Detector : KSETA Plenary Workshop, Durbach, KIT Die Forschungsuniversität in der Helmholtz-Gemeinschaft www.kit.edu Large Hadron Collider at CERN Since 2015: proton proton collisions @ 13 TeV Four experiments:

More information

RESULTS OF 3D PHOTOGRAMMETRY ON THE CMS BARREL YOKE

RESULTS OF 3D PHOTOGRAMMETRY ON THE CMS BARREL YOKE RESULTS OF 3D PHOTOGRAMMETRY ON THE CMS BARREL YOKE R. GOUDARD, C. HUMBERTCLAUDE *1, K. NUMMIARO CERN, European Laboratory for Particle Physics, Geneva, Switzerland 1. INTRODUCTION Compact Muon Solenoid

More information

Insertion Devices Lecture 4 Undulator Magnet Designs. Jim Clarke ASTeC Daresbury Laboratory

Insertion Devices Lecture 4 Undulator Magnet Designs. Jim Clarke ASTeC Daresbury Laboratory Insertion Devices Lecture 4 Undulator Magnet Designs Jim Clarke ASTeC Daresbury Laboratory Hybrid Insertion Devices Inclusion of Iron Simple hybrid example Top Array e - Bottom Array 2 Lines of Magnetic

More information

Strip Detectors. Principal: Silicon strip detector. Ingrid--MariaGregor,SemiconductorsasParticleDetectors. metallization (Al) p +--strips

Strip Detectors. Principal: Silicon strip detector. Ingrid--MariaGregor,SemiconductorsasParticleDetectors. metallization (Al) p +--strips Strip Detectors First detector devices using the lithographic capabilities of microelectronics First Silicon detectors -- > strip detectors Can be found in all high energy physics experiments of the last

More information

9/28/2010. Chapter , The McGraw-Hill Companies, Inc.

9/28/2010. Chapter , The McGraw-Hill Companies, Inc. Chapter 4 Sensors are are used to detect, and often to measure, the magnitude of something. They basically operate by converting mechanical, magnetic, thermal, optical, and chemical variations into electric

More information

Packaging of Cryogenic Components

Packaging of Cryogenic Components Packaging of Cryogenic Components William J. Schneider Senior Mechanical Engineer Emeritus November 19-23 2007 1 Packaging of Cryogenic Components Day one Introduction and Overview 2 What is important?

More information

8.882 LHC Physics. Detectors: Muons. [Lecture 11, March 11, 2009] Experimental Methods and Measurements

8.882 LHC Physics. Detectors: Muons. [Lecture 11, March 11, 2009] Experimental Methods and Measurements 8.882 LHC Physics Experimental Methods and Measurements Detectors: Muons [Lecture 11, March 11, 2009] Organization Project 1 (charged track multiplicity) no one handed in so far... well deadline is tomorrow

More information

SPECIFICATION FOR A 7.0 TESLA/400MM ROOM TEMPERATURE BORE MAGNET SYSTEM

SPECIFICATION FOR A 7.0 TESLA/400MM ROOM TEMPERATURE BORE MAGNET SYSTEM SPECIFICATION FOR A 7.0 TESLA/400MM ROOM TEMPERATURE BORE MAGNET SYSTEM Prepared by:- Magnex Scientific Limited The Magnet Technology Centre 6 Mead Road Oxford Industrial Park Yarnton, Oxford OX5 1QU,

More information

The CMS Outer HCAL SiPM Upgrade.

The CMS Outer HCAL SiPM Upgrade. The CMS Outer HCAL SiPM Upgrade. Artur Lobanov on behalf of the CMS collaboration DESY Hamburg CALOR 2014, Gießen, 7th April 2014 Outline > CMS Hadron Outer Calorimeter > Commissioning > Cosmic data Artur

More information

Cryogenic Operations at SLAC

Cryogenic Operations at SLAC Cryogenic Operations at SLAC J. G. Weisend II, A. Candia, W.W. Craddock, E. Thompson CryoOps 2006 5/30/2006 J. G. Weisend II 1 What Do We Do? Cryogenics at SLAC involve: Large scale He refrigerator operation

More information

Recommended Locations of Beam Loss Monitors for the ATLAS Roman Pots

Recommended Locations of Beam Loss Monitors for the ATLAS Roman Pots LHC Project Note 397 19 March 2007 Richard.Hall-Wilton@cern.ch Recommended Locations of Beam Loss Monitors for the ATLAS Roman Pots R.J.Hall-Wilton TS/LEA, D.Macina TS/LEA, V.Talanov TS/LEA Keywords: long

More information

To produce more powerful and high-efficiency particle accelerator, efforts have

To produce more powerful and high-efficiency particle accelerator, efforts have Measuring Unloaded Quality Factor of Superconducting RF Cryomodule Jian Cong Zeng Department of Physics and Astronomy, State University of New York at Geneseo, Geneseo, NY 14454 Elvin Harms, Jr. Accelerator

More information

Production of HPDs for the LHCb RICH Detectors

Production of HPDs for the LHCb RICH Detectors Production of HPDs for the LHCb RICH Detectors LHCb RICH Detectors Hybrid Photon Detector Production Photo Detector Test Facilities Test Results Conclusions IEEE Nuclear Science Symposium Wyndham, 24 th

More information

Stato del progetto RICH di LHCb. CSN1 Lecce, 24 settembre 2003

Stato del progetto RICH di LHCb. CSN1 Lecce, 24 settembre 2003 Stato del progetto RICH di LHCb CSN1 Lecce, 24 settembre 2003 LHCb RICH detectors Particle ID over 1 100 GeV/c provided by 2 RICH detectors RICH2: No major changes since RICH TDR PRR in february 2003 Superstructure

More information

The LHCb Vertex Locator : Marina Artuso, Syracuse University for the VELO Group

The LHCb Vertex Locator : Marina Artuso, Syracuse University for the VELO Group The LHCb Vertex Locator : status and future perspectives Marina Artuso, Syracuse University for the VELO Group The LHCb Detector Mission: Expore interference of virtual new physics particle in the decays

More information

CERN (The European Laboratory for Particle Physics)

CERN (The European Laboratory for Particle Physics) 462 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 48, NO. 2, APRIL 1999 The Measurement Challenge of the LHC Project Gunnar Fernqvist Abstract In 2005, CERN is planning to commission its next

More information

XFEL Cryo System. Project X Collaboration Meeting, FNAL September 8-9, 2010 Bernd Petersen DESY MKS (XFEL WP10 & WP13) 1 st stage. Possible extension

XFEL Cryo System. Project X Collaboration Meeting, FNAL September 8-9, 2010 Bernd Petersen DESY MKS (XFEL WP10 & WP13) 1 st stage. Possible extension XFEL Cryo System Possible extension 1 st stage Project X Collaboration Meeting, FNAL September 8-9, 2010 (XFEL WP10 & WP13) Outline 2 XFEL accelerator structure TESLA technology Basic cryogenic parameters

More information

High Voltage Instrumentation Cables for the ITER Superconducting Magnet Systems

High Voltage Instrumentation Cables for the ITER Superconducting Magnet Systems High Voltage Instrumentation Cables for the ITER Superconducting Magnet Systems Summary for Call for Nominations 1. Background and scope ITER will be the world's largest experimental facility to demonstrate

More information

Vertex Detector Mechanics

Vertex Detector Mechanics Vertex Detector Mechanics Bill Cooper Fermilab (Layer 5) (Layer 1) VXD Introduction The overall approach to mechanical support and cooling has been developed in conjunction with SiD. The support structures

More information

Cryogenic Testing of Superconducting Corrector Magnets for the LHC Main Dipole

Cryogenic Testing of Superconducting Corrector Magnets for the LHC Main Dipole Cryogenic Testing of Superconducting Corrector Magnets for the LHC Main Dipole A.M. Puntambekar SC Tech Lab, AAMD Div. Raja Ramanna Centre For Advanced Technology, Indore Workshop on Cryogenic Science

More information

TEST AND CALIBRATION FACILITY FOR HLS AND WPS SENSORS

TEST AND CALIBRATION FACILITY FOR HLS AND WPS SENSORS IWAA2004, CERN, Geneva, 4-7 October 2004 TEST AND CALIBRATION FACILITY FOR HLS AND WPS SENSORS Andreas Herty, Hélène Mainaud-Durand, Antonio Marin CERN, TS/SU/MTI, 1211 Geneva 23, Switzerland 1. ABSTRACT

More information

The Commissioning of the ATLAS Pixel Detector

The Commissioning of the ATLAS Pixel Detector The Commissioning of the ATLAS Pixel Detector XCIV National Congress Italian Physical Society Genova, 22-27 Settembre 2008 Nicoletta Garelli Large Hadronic Collider MOTIVATION: Find Higgs Boson and New

More information

The LHCb Upgrade BEACH Simon Akar on behalf of the LHCb collaboration

The LHCb Upgrade BEACH Simon Akar on behalf of the LHCb collaboration The LHCb Upgrade BEACH 2014 XI International Conference on Hyperons, Charm and Beauty Hadrons! University of Birmingham, UK 21-26 July 2014 Simon Akar on behalf of the LHCb collaboration Outline The LHCb

More information

ATLAS strip detector upgrade for the HL-LHC

ATLAS strip detector upgrade for the HL-LHC ATL-INDET-PROC-2015-010 26 August 2015, On behalf of the ATLAS collaboration Santa Cruz Institute for Particle Physics, University of California, Santa Cruz E-mail: zhijun.liang@cern.ch Beginning in 2024,

More information

Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator

Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator Every accelerator needs a linac as injector to pass the region where the velocity of the particles increases with energy. At high energies (relativity)

More information

Improving seismic isolation in Advanced LIGO using a ground rotation sensor

Improving seismic isolation in Advanced LIGO using a ground rotation sensor Improving seismic isolation in Advanced LIGO using a ground rotation sensor 04/16/2016 Krishna Venkateswara for UW- Michael Ross, Charlie Hagedorn, and Jens Gundlach aligo SEI team LIGO-G1600083 1 Contents

More information

Construction and Performance of the stgc and Micromegas chambers for ATLAS NSW Upgrade

Construction and Performance of the stgc and Micromegas chambers for ATLAS NSW Upgrade Construction and Performance of the stgc and Micromegas chambers for ATLAS NSW Upgrade Givi Sekhniaidze INFN sezione di Napoli On behalf of ATLAS NSW community 14th Topical Seminar on Innovative Particle

More information

Status of the LHCb Experiment

Status of the LHCb Experiment Status of the LHCb Experiment Werner Witzeling CERN, Geneva, Switzerland On behalf of the LHCb Collaboration Introduction The LHCb experiment aims to investigate CP violation in the B meson decays at LHC

More information

BL39XU Magnetic Materials

BL39XU Magnetic Materials BL39XU Magnetic Materials BL39XU is an undulator beamline that is dedicated to hard X-ray spectroscopy and diffractometry requiring control of the X-ray polarization state. The major applications of the

More information

The Inner Tracker detector of the LHCb experiment.

The Inner Tracker detector of the LHCb experiment. The Inner Tracker detector of the LHCb exeriment. CERN and LHC LHCb detector Inner Tracker EPFL CERN and LHC Large Hadron Collider * collisions * 7 TeV er beam 4 exeriments: CMS & Atlas Alice and LHCb

More information

Metrology Studies and Baseplate-Pixel Sensor Gluing of the Pixel Strip Modules for the CMS II Phase Upgrade

Metrology Studies and Baseplate-Pixel Sensor Gluing of the Pixel Strip Modules for the CMS II Phase Upgrade Metrology Studies and Baseplate-Pixel Sensor Gluing of the Pixel Strip Modules for the CMS II Phase Upgrade Author: Jem Aizen M. Guhit Supervisors: James Keaveney Marino Missiroli Abstract The upcoming

More information

Commissioning of Advanced Virgo

Commissioning of Advanced Virgo Commissioning of Advanced Virgo VSR1 VSR4 VSR5/6/7? Bas Swinkels, European Gravitational Observatory on behalf of the Virgo Collaboration GWADW Takayama, 26/05/2014 B. Swinkels Adv. Virgo Commissioning

More information

Supplementary Figure 1

Supplementary Figure 1 Supplementary Figure 1 Technical overview drawing of the Roadrunner goniometer. The goniometer consists of three main components: an inline sample-viewing microscope, a high-precision scanning unit for

More information

+++ construction manual SR 71 Blackbird (EDF Version) from JetCom +++

+++ construction manual SR 71 Blackbird (EDF Version) from JetCom +++ Table of content: Page List of material and overview of provided frames 3 Mounting of main gear 4 Mounting of nose gear 5 Mounting of elevons 6 Installation of the rudders 7 Mounting of the rudders 9 Installation

More information

Physical Properties Measurement System (PPMS): Detailed specifications: Basic unit cryogen- free

Physical Properties Measurement System (PPMS): Detailed specifications: Basic unit cryogen- free Physical Properties Measurement System (PPMS): A Cryogen-free Physical Properties Measurement system that operates over a wider range of temperature and magnetic fields: fully automated/computer controlled

More information

SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS. An Energetic Kick. Having a Worldwide Impact

SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS. An Energetic Kick. Having a Worldwide Impact Frank DiMeo SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS An Energetic Kick A key component of any modern particle accelerator is the electromagnetic cavity resonator. Inside the hollow resonator

More information

200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm

200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm M. Vretenar, CERN for the HF-RFQ Working Group (V.A. Dimov, M. Garlasché, A. Grudiev, B. Koubek, A.M. Lombardi, S. Mathot, D. Mazur, E. Montesinos, M. Timmins, M. Vretenar) 1 1988-92 Linac2 RFQ2 202 MHz

More information

Micro-manipulated Cryogenic & Vacuum Probe Systems

Micro-manipulated Cryogenic & Vacuum Probe Systems Janis micro-manipulated probe stations are designed for non-destructive electrical testing using DC, RF, and fiber-optic probes. They are useful in a variety of fields including semiconductors, MEMS, superconductivity,

More information

The HERA-B Ring Imaging Cerenkov ˇ Detector

The HERA-B Ring Imaging Cerenkov ˇ Detector The HERA-B Ring Imaging Cerenkov ˇ Detector Requirements Physics Genova, July 3, 1998 Jörg Pyrlik University of Houston HERA-B Collaboration Space Limitations Rate Capabilities and Aging Design Radiator

More information

COIL WINDING ISSUES P. Fabbricatore INFN Genova LCD - Magnet 13Oct09. Coil winding issues

COIL WINDING ISSUES P. Fabbricatore INFN Genova LCD - Magnet 13Oct09. Coil winding issues Coil winding issues Based on experience acquired with CMS coil construction, some preliminary considerations about the envisaged winding (and in general manufacturing) issues of a large superconducting

More information

MULTIPACTING IN THE CRAB CAVITY

MULTIPACTING IN THE CRAB CAVITY MULTIPACTING IN TH CRAB CAVITY Y. Morita, K. Hara, K. Hosoyama, A. Kabe, Y. Kojima, H. Nakai, KK, 1-1, Oho, Tsukuba, Ibaraki 3-81, JAPAN Md. M. Rahman, K. Nakanishi, Graduate University for Advanced Studies,

More information

DQW HOM Coupler for LHC

DQW HOM Coupler for LHC DQW HOM Coupler for LHC J. A. Mitchell 1, 2 1 Engineering Department Lancaster University 2 BE-RF-BR Section CERN 03/07/2017 J. A. Mitchell (PhD Student) HL LHC UK Jul 17 03/07/2017 1 / 27 Outline 1 LHC

More information

Photonics in Particle Physics

Photonics in Particle Physics Photonics in Particle Physics Prof. Peter R Hobson C.Phys M.Inst.P. School of Engineering and Design Brunel University, Uxbridge Updated December 2014 Peter.Hobson@brunel.ac.uk What is Photonics The technology

More information

Review of the magnetic measurement technique (experience of the SLC, LEP, CEBAF)

Review of the magnetic measurement technique (experience of the SLC, LEP, CEBAF) Review of the magnetic measurement technique (experience of the SLC, LEP, CEBAF) N.A.Morozov Workshop on the TESLA spectrometer, Dubna, 13-14 October 2003 1..Stanford Linear Collider (SLC) To implement

More information

MRI SYSTEM COMPONENTS Module One

MRI SYSTEM COMPONENTS Module One MRI SYSTEM COMPONENTS Module One 1 MAIN COMPONENTS Magnet Gradient Coils RF Coils Host Computer / Electronic Support System Operator Console and Display Systems 2 3 4 5 Magnet Components 6 The magnet The

More information

SURVEY AND ALIGNMENT FOR THE SWISS LIGHT SOURCE

SURVEY AND ALIGNMENT FOR THE SWISS LIGHT SOURCE 1 SURVEY AND ALIGNMENT FOR THE SWISS LIGHT SOURCE F.Q. Wei, K. Dreyer, U. Fehlmann, J.L. Pochon and A. Wrulich SLS / Paul Scherrer Institute CH5232 Villigen PSI Switzerland ABSTRACT The Swiss Light Source

More information

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

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS CR -2015/213 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 05 October 2015 (v2, 12 October 2015)

More information

TECHNICAL SPECIFICATIONS. FOR AN MRBR 7.0 TESLA / 160mm ACTIVELY SHIELDED ROOM TEMPERATURE BORE MAGNET SYSTEM

TECHNICAL SPECIFICATIONS. FOR AN MRBR 7.0 TESLA / 160mm ACTIVELY SHIELDED ROOM TEMPERATURE BORE MAGNET SYSTEM TECHNICAL SPECIFICATIONS FOR AN MRBR 7.0 TESLA / 160mm ACTIVELY SHIELDED ROOM TEMPERATURE BORE MAGNET SYSTEM Prepared by:- Magnex Scientific Limited The Magnet Technology Centre 6 Mead Road Oxford Industrial

More information

What do the experiments want?

What do the experiments want? What do the experiments want? prepared by N. Hessey, J. Nash, M.Nessi, W.Rieger, W. Witzeling LHC Performance Workshop, Session 9 -Chamonix 2010 slhcas a luminosity upgrade The physics potential will be

More information

Lecture 11. Complex Detector Systems

Lecture 11. Complex Detector Systems Lecture 11 Complex Detector Systems 1 Dates 14.10. Vorlesung 1 T.Stockmanns 1.10. Vorlesung J.Ritman 8.10. Vorlesung 3 J.Ritman 04.11. Vorlesung 4 J.Ritman 11.11. Vorlesung 5 J.Ritman 18.11. Vorlesung

More information

HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY

HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY G. Devanz, D. Braud, M. Desmons, Y. Gasser, E. Jacques, O. Piquet, J. Plouin, J.- P. Poupeau, D. Roudier, P. Sahuquet, CEA-Saclay,

More information

Recent work on Hall A magnets Present and future Jay Benesch January 2018

Recent work on Hall A magnets Present and future Jay Benesch January 2018 Recent work on Hall A magnets Present and future Jay Benesch January 2018 1 Sources All of the information contained herein can be found in much more detail in the following Tech Notes: 16-043 (SoLID),

More information

Roman Pots. Marco Oriunno SLAC, PPA. M.Oriunno, SLAC

Roman Pots. Marco Oriunno SLAC, PPA. M.Oriunno, SLAC Roman Pots Marco Oriunno SLAC, PPA The Roman Pot technique 1. The Roman Pot, an historically successful technique for near beam physics: ISR, SPS, TEVATRON, RICH, DESY 2. A CERN in-house technology: ISR,

More information

PoS(EPS-HEP2017)476. The CMS Tracker upgrade for HL-LHC. Sudha Ahuja on behalf of the CMS Collaboration

PoS(EPS-HEP2017)476. The CMS Tracker upgrade for HL-LHC. Sudha Ahuja on behalf of the CMS Collaboration UNESP - Universidade Estadual Paulista (BR) E-mail: sudha.ahuja@cern.ch he LHC machine is planning an upgrade program which will smoothly bring the luminosity to about 5 34 cm s in 228, to possibly reach

More information

2. Refraction and Reflection

2. Refraction and Reflection 2. Refraction and Reflection In this lab we will observe the displacement of a light beam by a parallel plate due to refraction. We will determine the refractive index of some liquids from the incident

More information

Testing of the Toroidal Field Model Coil (TFMC)

Testing of the Toroidal Field Model Coil (TFMC) 1 CT/P 14 Testing of the Toroidal Field Model Coil (TFMC) E. Salpietro on behalf of the ITER-TFMC Team EFDA-CSU, Garching,, Germany ettore.salpietro@tech.efda.org Abstract The paper shortly describes the

More information

PoS(VERTEX2015)008. The LHCb VELO upgrade. Sophie Elizabeth Richards. University of Bristol

PoS(VERTEX2015)008. The LHCb VELO upgrade. Sophie Elizabeth Richards. University of Bristol University of Bristol E-mail: sophie.richards@bristol.ac.uk The upgrade of the LHCb experiment is planned for beginning of 2019 unitl the end of 2020. It will transform the experiment to a trigger-less

More information

The CMS Silicon Strip Tracker and its Electronic Readout

The CMS Silicon Strip Tracker and its Electronic Readout The CMS Silicon Strip Tracker and its Electronic Readout Markus Friedl Dissertation May 2001 M. Friedl The CMS Silicon Strip Tracker and its Electronic Readout 2 Introduction LHC Large Hadron Collider:

More information

INDUSTRIAL CONTROLS FOR TEST SYSTEMS FROM SUPERCONDUCTING STRANDS TILL MAGNET FIDUCIALISATION IN THE TUNNEL FOR THE LHC PROJECT

INDUSTRIAL CONTROLS FOR TEST SYSTEMS FROM SUPERCONDUCTING STRANDS TILL MAGNET FIDUCIALISATION IN THE TUNNEL FOR THE LHC PROJECT INDUSTRIAL CONTROLS FOR TEST SYSTEMS FROM SUPERCONDUCTING STRANDS TILL MAGNET FIDUCIALISATION IN THE TUNNEL FOR THE LHC PROJECT ABSTRACT A. Rijllart, C. Charrondière, B. Khomenko, M. Marchesotti, E. Michel,

More information

Magnetic measurement system for superconducting final focus quadrupoles for SuperKEKB

Magnetic measurement system for superconducting final focus quadrupoles for SuperKEKB Magnetic measurement system for superconducting final focus quadrupoles for SuperKEKB Y. Arimoto (KEK) IMMW 20 @ Diamond Light Source 2017/Jun/8 SuperKEKB Final focus magnet system Magnetic field measurement

More information

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT G. Olry, J-L. Biarrotte, S. Blivet, S. Bousson, C. Commeaux, C. Joly, T. Junquera, J. Lesrel, E. Roy,

More information

AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Milestone Report

AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Milestone Report AIDA-2020-MS15 AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators Milestone Report Design specifications of test stations for irradiated silicon sensors and LHC oriented front-end

More information

Mosca-Genova: SMART CITY futuro o realtà?

Mosca-Genova: SMART CITY futuro o realtà? ASG @ Mosca-Genova: SMART CITY futuro o realtà? www.asgsuperconductors.com ASG AND COMPANIES OF THE MALACALZA FAMILY www.asgsuperconductors.com 2 ASG: A GLIMPSE OF THE GENOA WORKS www.asgsuperconductors.com

More information

PRELIMINARY SPECIFICATIONS MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED CRYO-COOLED MAGNET SYSTEM

PRELIMINARY SPECIFICATIONS MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED CRYO-COOLED MAGNET SYSTEM PRELIMINARY SPECIFICATIONS MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED CRYO-COOLED MAGNET SYSTEM Prepared by:- Magnex Scientific Limited The Magnet Technology Centre 6 Mead Road Oxford Industrial Park Yarnton,

More information

A novel solution for various monitoring applications at CERN

A novel solution for various monitoring applications at CERN A novel solution for various monitoring applications at CERN F. Lackner, P. H. Osanna 1, W. Riegler, H. Kopetz CERN, European Organisation for Nuclear Research, CH-1211 Geneva-23, Switzerland 1 Department

More information

SPECIFICATIONS FOR AN MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED MAGNET SYSTEM

SPECIFICATIONS FOR AN MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED MAGNET SYSTEM SPECIFICATIONS FOR AN MRBR 7.0 TESLA / 210MM ACTIVELY SHIELDED MAGNET SYSTEM Prepared by:- Magnex Scientific Limited The Magnet Technology Centre 6 Mead Road Oxford Industrial Park Yarnton, Oxford OX5

More information

The LHCb VELO Upgrade. Stefano de Capua on behalf of the LHCb VELO group

The LHCb VELO Upgrade. Stefano de Capua on behalf of the LHCb VELO group The LHCb VELO Upgrade Stefano de Capua on behalf of the LHCb VELO group Overview [J. Instrum. 3 (2008) S08005] LHCb / Current VELO / VELO Upgrade Posters M. Artuso: The Silicon Micro-strip Upstream Tracker

More information

NON-TRADITIONAL MACHINING PROCESSES ULTRASONIC, ELECTRO-DISCHARGE MACHINING (EDM), ELECTRO-CHEMICAL MACHINING (ECM)

NON-TRADITIONAL MACHINING PROCESSES ULTRASONIC, ELECTRO-DISCHARGE MACHINING (EDM), ELECTRO-CHEMICAL MACHINING (ECM) NON-TRADITIONAL MACHINING PROCESSES ULTRASONIC, ELECTRO-DISCHARGE MACHINING (EDM), ELECTRO-CHEMICAL MACHINING (ECM) A machining process is called non-traditional if its material removal mechanism is basically

More information

Technology Workpieces and processes in the automotive industry

Technology Workpieces and processes in the automotive industry Technology Workpieces and processes in the automotive industry New machining solutions for that extra productivity and cost-effectiveness MAPAL technology: Tap the potential savings during the machining

More information

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team Engineering Challenges and Solutions for MeRHIC Andrew Burrill for the MeRHIC Team Key Components Photoinjector Design Photocathodes & Drive Laser Linac Cavities 703.75 MHz 5 cell cavities 3 rd Harmonic

More information

The Superconducting Strand for the CMS Solenoid Conductor

The Superconducting Strand for the CMS Solenoid Conductor The Superconducting Strand for the CMS Solenoid Conductor B. Curé, B. Blau, D. Campi, L. F. Goodrich, I. L. Horvath, F. Kircher, R. Liikamaa, J. Seppälä, R. P. Smith, J. Teuho, and L. Vieillard Abstract-

More information

Micromegas calorimetry R&D

Micromegas calorimetry R&D Micromegas calorimetry R&D June 1, 214 The Micromegas R&D pursued at LAPP is primarily intended for Particle Flow calorimetry at future linear colliders. It focuses on hadron calorimetry with large-area

More information

RD51 ANNUAL REPORT WG1 - Technological Aspects and Development of New Detector Structures

RD51 ANNUAL REPORT WG1 - Technological Aspects and Development of New Detector Structures RD51 ANNUAL REPORT 2009 WG1 - Technological Aspects and Development of New Detector Structures Conveners: Serge Duarte Pinto (CERN), Paul Colas (CEA Saclay) Common projects Most activities in WG1 are meetings,

More information

Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission

Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission Pardis Niknejadi California State Polytechnic University, Pomona, CA 91768 Elizabeth Olhsson University of Oregon, Eugene, OR

More information

QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER*

QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER* QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER* P.N. Prakash and A.Roy Nuclear Science Centre, P.O.Box 10502, New Delhi 110 067, INDIA and K.W.Shepard Physics Division, Argonne National Laboratory,

More information

DEVELOPMENT OF OFFNER RELAY OPTICAL SYSTEM FOR OTR MONITOR AT 3-50 BEAM TRANSPORT LINE OF J-PARC

DEVELOPMENT OF OFFNER RELAY OPTICAL SYSTEM FOR OTR MONITOR AT 3-50 BEAM TRANSPORT LINE OF J-PARC Proceedings of IBIC01, Tsukuba, Japan DEVELOPMENT OF OFFNER RELAY OPTICAL SYSTEM FOR OTR MONITOR AT 3-50 BEAM TRANSPORT LINE OF J-PARC M. Tejima #, Y. Hashimoto, T. Toyama, KEK/J-PARC, Tokai, Ibaraki,

More information

SIMULATION OF A SIGNAL IN THE BEAM LOSS

SIMULATION OF A SIGNAL IN THE BEAM LOSS RADIATION ASPECTS OF LHC SIMULATION OF A SIGNAL IN THE BEAM LOSS MONITORS OF THE MOMENTUM CLEANING INSERTION FOR THE NEW COLLIMATOR JAWS DESIGN IHEP, Protvino, Russia Summary of the presentation Page 1

More information

ATLAS NSW Alignment System. Study on Inductors

ATLAS NSW Alignment System. Study on Inductors ATLAS NSW Alignment System Study on Inductors Senior Thesis Presented to Faculty of the School of Arts and Sciences Brandeis University Undergraduate Program in Physics by Cheng Li Advisor: James Bensinger

More information

`First ep events in the Zeus micro vertex detector in 2002`

`First ep events in the Zeus micro vertex detector in 2002` Amsterdam 18 dec 2002 `First ep events in the Zeus micro vertex detector in 2002` Erik Maddox, Zeus group 1 History (1): HERA I (1992-2000) Lumi: 117 pb -1 e +, 17 pb -1 e - Upgrade (2001) HERA II (2001-2006)

More information

First data from the ATLAS Inner Detector FSI Alignment System

First data from the ATLAS Inner Detector FSI Alignment System KEK, Tsukuba, Japan. 15 February 2008. First data from the ATLAS Inner Detector FSI Alignment System S. M. Gibson, P. A. Coe*, M. Dehchar, J. Fopma, D.F. Howell, R. B. Nickerson, G. Viehhauser Particle

More information

The ATLAS detector at the LHC

The ATLAS detector at the LHC The ATLAS detector at the LHC Andrée Robichaud-Véronneau on behalf of the ATLAS collaboration Université de Genève July 17th, 2009 Abstract The world s largest multi-purpose particle detector, ATLAS, is

More information

Spectrometer cavern background

Spectrometer cavern background ATLAS ATLAS Muon Muon Spectrometer Spectrometer cavern cavern background background LPCC Simulation Workshop 19 March 2014 Jochen Meyer (CERN) for the ATLAS Collaboration Outline ATLAS Muon Spectrometer

More information

attocube systems Probe Stations for Extreme Environments CRYOGENIC PROBE STATION fundamentals principles of cryogenic probe stations

attocube systems Probe Stations for Extreme Environments CRYOGENIC PROBE STATION fundamentals principles of cryogenic probe stations PAGE 88 & 2008 2007 PRODUCT CATALOG CRYOGENIC PROBE STATION fundamentals...................... 90 principles of cryogenic probe stations attocps I.......................... 92 ultra stable cryogenic probe

More information

Status Report. Design report of a 3 MW power amplifier

Status Report. Design report of a 3 MW power amplifier TIARA-REP-WP7-2014-005 Test Infrastructure and Accelerator Research Area Status Report Design report of a 3 MW power amplifier Montesinos, E. (CERN) et al 10 February 2014 The research leading to these

More information