Muon Ionization Cooling Experiment - MICE HEPTech - Grenoble 4-5 th June 2015 Tom Bradshaw STFC, Rutherford Appleton Laboratory.

Slides:



Advertisements
Similar presentations
1 paul drumm; Jan’05; MICE RF Needs MICE RF Power Paul Drumm ISIS Facility Rutherford Appleton Laboratory & MICE.
Advertisements

Progress in the construction of the MICE cooling channel and first measurements Adam Dobbs, EPS-HEP, 23 rd July 2011.
Status of the AFC at RAL Tom Bradshaw John Cobb Wing Lau Matt Hills Elwyn Baynham Mike Courthold Victoria Bayliss MICE Project Board 28 th June 2011.
ISIS Related Issues for MICE Adam Dobbs Proton Accelerator Development Meeting, RAL 24 th March /03/20111A. Dobbs.
MICE Superconducting Solenoids: Status and Update RAL: T W Bradshaw M Courthold J Rochford M Hills D Baynham Oxford: J Cobb W Lau S Yang MICE.
Magnet quench during a training run Magnet electrical circuit schematic PROGRESS ON THE MODELING AND MODIFICATION OF THE MICE SUPERCONDUCTING SPECTROMETER.
Cryogenic Technology from STFC Cryox Ltd was formed in 2007 to provide a commercial face for cryogenic technology from the three main.
Progress on the MICE Cooling Channel Solenoid Magnet System
Changing the absorbers: how does it fit in the MICE experimental programme? Besides the requirement that the amount of multiple scattering material be.
1 MICE Mtg Oct 2002 Elwyn Baynham RAL Focussing Absorber Magnet Elwyn Baynham ; Tom Bradshaw Iouri Ivaniouchenkov ; Jim Rochford Applied Science Division.
March 2003 Paul Drumm MICE Collaboration Meeting, CERN 1 Beam Line & Installation Plans Paul Drumm CLRC Rutherford Appleton Laboratory.
Report from meeting Hydrogen system operation from cryocooler and level control Cryocoolers for MICE Tom Bradshaw Elwyn Baynham Yury Ivanyushenkov Rutherford.
9 June 2006MICE CM-15 Fermilab1 Progress on the MICE Cooling Channel and Tracker Magnets since CM-14 Michael A. Green Lawrence Berkeley Laboratory.
1 Superconducting Magnets for the MICE Channel Michael A. Green Oxford University Physics Department Oxford OX1-3RH, UK.
1 Progress on the MICE Cooling Channel Magnets Michael A. Green Lawrence Berkeley National Laboratory 28 June 2005.
DPNC Sept 2007Jean-Sébastien Graulich MICE The international Muon Ionization Cooling Experiment o o Introduction o o Beam Line o o Cooling Channel o o.
Overview of Experiment and Parameter Choices presented by Giles Barr.
MICE Hydrogen System Design Tom Bradshaw Iouri Ivaniouchenkov Elwyn Baynham Columbia Meeting June 2003.
Progress on the MuCool and MICE Coupling Coils * L. Wang a, X. K Liu a, F. Y. Xu a, A. B. Chen a, H. Pan a, H. Wu a, X. L. Guo a, S. X Zheng a, D. Summers.
Neutrino Factory Workshop UK Magnet Manufacturing Capability Elwyn Baynham CCLRC Rutherford Appleton Laboratory, UK Elwyn Baynham UKNF Oct 2003.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices iteratively to determine trace.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices to map  path Assume straight.
Magnet quench during a training run Successfully trained to peak currents and operationally tested Thermal performance requirements met 3D magnetic bore.
The MICE demonstration of ionization cooling J. Pasternak #, V. Blackmore, C. Hunt, J-B. Lagrange, K. Long, Imperial College, London, UK Alain Blondel,
(+) session, PAC09 Vancouver – TH6PFP056 Introduction The Muon Ionisation Cooling Experiment (MICE, fig. 1c) at RAL[1]
Goals and Status of MICE The International Muon Ionization Cooling Experiment J.S. Graulich.
Particle Production in the MICE Beam Line Particle Accelerator Conference, May 2009, Vancouver, Canada Particle Production in the MICE Beam Line Jean-Sebastien.
Paul Soler University of Glasgow MICE as a Step towards Cool Muon Beams for Particle Physics MICE Celebration Event RAL, 25 June 2015.
The status of the construction of MICE Step IV K. Long, on behalf of the MICE collaboration.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
ICHEP 2012 Melbourne, 7 July 2012 Paul Soler on behalf of the MICE Collaboration The MICE Beam Line Instrumentation (Trackers and PID) for precise Emittance.
MICE VC Alain Blondel 1 MICE NEWS MICE VC Next Collaboration meeting will be Jun at IIT and the 19th at Fermilab right before the.
Status of the MICE Project & Dashboard MICE Project Board 14 th November 2013 Roy Preece.
Abstract: The Muon Ionization Cooling Experiment (MICE) is an international effort sited at Rutherford Appleton Laboratory, which will demonstrate ionization.
Particle Production in the MICE Beamline IPAC10 Linda Coney, UC Riverside, Adam Dobbs, Imperial College London, Yordan Karadzhov, Sofia University The.
MICE at STFC-RAL The International Muon Ionization Cooling Experiment -- Design, engineer and build a section of cooling channel capable of giving the.
Magnet vacuum vessel w/radiation shield and cold mass in place Magnet leads (left) and the three cryocoolers on the top of the spectrometer solenoid service.
Project Managers Report CM40 Collaboration Board – Rome Roy Preece 28 th October 2014.
MICE CC visit at CERN Alain Blondel 1   MICE The International Muon Ionization Cooling Experiment.
MICE: The International Muon Ionisation Cooling Experiment MOPLT106 Abstract The provision of intense stored muon beams would allow the properties of neutrinos.
MPB 31 October 2012 and FAC 15 November monitor how well we are doing in assembling step IV ! -- should deliver a ‘realsitic schedule scenario’
MICE Oversight Committee Meeting RAL, 24 April 2014 Paul Soler on behalf of the MICE Collaboration Status of MICE and Spectrometer Solenoids.
MICE FAC open session Alain Blondel 1   MICE The International Muon Ionization Cooling Experiment.
Timing measurements at the MICE experiment – 1 The analysis of timing measurements at the Muon Ionization Cooling Experiment Mark Rayner The University.
Progress in the construction of the MICE cooling channel and first measurements Adam Dobbs, EPS-HEP, 23 rd July 2011.
MICE hydrogen review Introduction to MICE. After the LHC… Many open questions in physics: Gravity & standard model Matter-antimatter imbalance Dark matter.
CHIPP Aug 2010J.S. GraulichSlide 1 MICE and the Neutrino Factory Jean-Sebastien Graulich, Geneva.
- MICE - The Muon Ionization Cooling Experiment Jean-Sebastien Graulich, Univ. Genève o Introduction: Aims And Concept o Design o Infrastructure: Hall,
CHIPP Oct 2007Jean-Sébastien Graulich Status of MICE Jean-Sebastien Graulich, Univ. Genève o o Introduction o o Beam Line o o Technical Design o o PID.
Progress on MICE RFCC Module for the MICE Experiment * Allan DeMello, Nord Andresen, Michael Green, Derun Li, Heng Pan, Steve Virostek, Michael Zisman.
1 UK Project Roy Preece – STFC Alan Grant, STFC. Finance Staffing Update on stepIV position Milestones Critical Path – stepIV Magnetic field mitigation.
(one of the) Request from MPB
MICE S TEP IV P HYSICS ‘D ELIVERABLES ’ V. Blackmore MAP 2014 Spring Meeting 30 th May, /15 AKA “What will we learn from Step IV?”
Muons, Inc. Feb Yonehara-AAC AAC Meeting Design of the MANX experiment Katsuya Yonehara Fermilab APC February 4, 2009.
K. Long, 28 June, 2016 Introduction to MICE — and the role of the Hydrogen Delivery System.
MICE. Outline Experimental methods and goals Beam line Diagnostics – In HEP parlance – the detectors Magnet system 2MICE Optics Review January 14, 2016.
MICE Step IV Commissioning: Overview (March-April 2015) Milorad Popovic MAP 2015 Spring Collaboration Meeting.
EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement Ionisation Cooling Test.
Research and development toward a future Muon Collider Katsuya Yonehara Accelerator Physics Center, Fermilab On behalf of Muon Accelerator Program Draft.
Refrigeration of Superconducting Solenoids T W Bradshaw Rutherford Appleton Laboratory Harwell Science and Innovation Campus Didcot, OX11 0QX, UK
MICE. Outline Experimental methods and goals Beam line Diagnostics – In HEP parlance – the detectors Magnet system 2MICE Optics Review January 14, 2016.
MICE Absorber and Focus Coil Magnet – Test Results
Muon Ionisation Cooling Experiment Overview
Status of the MICE Construction Project
An introduction to MICE
On the Ground Muon Ionisation Cooling Experiment ( MICE ) – pre-cursor to a neutrino factory.
MICE The International Muon Ionisation Cooling Experiment
Design of the MANX experiment
K. Tilley, ISIS, Rutherford Appleton Laboratory, UK Introduction
The Detector System of the MICE Experiment
Presentation transcript:

Muon Ionization Cooling Experiment - MICE HEPTech - Grenoble 4-5 th June 2015 Tom Bradshaw STFC, Rutherford Appleton Laboratory

Rationale The Muon Ionization Cooling Experiment (MICE) is being built by an international consortium to demonstrate part of the technology required to build a neutrino factory. Neutrinos are very poorly understood subatomic particles that are generated in radioactive decay and in nuclear processes in the Sun. Get about 10,000/m 2 /min on earth from cosmic ray interactions Muons are a sub atomic particle similar to an electron but with a heavier mass. These decay into an electron and two neutrinos after 2.2µs. The experiment aims to show that muons can be controlled and focused into a beam ready for use in a neutrino factory – other uses could be for a Muon Collider.

Bulgaria – Science China - magnets Italy – Cherenkov detectors, EMR Japan – Absorber France - Tracker Serbia - Science Switzerland & CERN – Decay Solenoid, EMR detector, RF components, Magnet measurement UK – hosting experiment, Absorber and Focus Coil, Tracker, Diffuser, RF, Controls, Hydrogen System USA – Spectrometer Solenoids, RF components An International Experiment

What is ionization cooling? The divergent beam of muons collide with atomic electrons (ionization bit..) slowing them down reducing the momentum They are then re-accelerated in the forward direction Repeat until beam is focused to the required degree –“Decrease of transverse emittance” –Do get heating from the scattering – need to keep this low

MICE Overview A Titanium target is dipped into the ISIS proton beamline Decay products enter Decay Solenoid – unwanted particles are steered away from the beam line Quadrupoles steer the (divergent beam of) muons into the MICE lattice This part is the MICE Beamline – this generates the muon beam that will be studied…

MICE Overview Spectrometer solenoid has trackers to measure energy and direction of the particles before and after the cooling process – hence the emittance (or divergence) of the beam can be measured – we are testing the lattice as a function of absorber, magnet and beam settings. An upstream diffuser consists of four irises made from brass and Tungsten to increase the emittance Beam

Decay Solenoid From Paul Scherrer Institute in Switzerland – made by Brown Boveri early 1970s There are ten separate “spools” that make up the magnet 5m length Transported to RAL and assembled into beam line Uses supercritical Helium to cool the spools load about 25W – quenches are completely undramatic

Decay Solenoid Leads are gas cooled with a flow of ~0.1g/s Operated at RAL with a current of 870Amps, 5T central field Cu:NbTi ratio of 3.5, conductor 1.5 x 3mm – very conservative design

Decay Solenoid Cryogenics provided by a Linde LR70 refrigerator Magnet unusually uses supercritical helium

The MICE Lattice The rest of the MICE lattice has magnets that are cooled using cryocoolers The decision was taken to go down this route as it meant that the individual magnets could be tested at the host institution prior to delivery The MICE lattice has to be reconfigured several times and it was felt that this would be easier with cryocoolers rather than a central helium plant and a network of transfer lines

Spectrometer Solenoids Built at Wang NMR in California – supplied by Lawrence Berkeley National Laboratory Two of these are used either side of the absorber. “Tracker” detectors are located inside the bore These are a complicated magnetic structure – 5 coils This is the most complicated of the MICE coils 1 x centre coil 2 x end coils 2 x matching coils

Spectrometer Solenoids The five coils are wound on a common Al bobbin Cryocoolers used to maintain liquid helium in a zero boil-off system 5 x two stage and one single stage There are a large number of current leads - challenging design

Absorber and Focus Coil Module The Absorber and Focus Coil Module is a split pair magnet These can be run in opposition (flip mode) or together (solenoid mode) At the centre is the 22litres of liquid hydrogen or the Lithium Hydride absorber

Absorber and Focus Coil Module Magnet was built by Tesla Engineering to a basic design provided by the collaboration Two were made – the first module took ~16 training cycles but the second only took 1 Magnets are split pairs but can be operated with field reversal or in solenoid mode

Control of the magnetic Field The partial return Yoke (PRY) sits outside the magnets and controls the stray magnetic field Consists of 55t of iron

Conclusions and Summary The MICE magnets have all been individually proved and are being assembled into the MICE lattice. The decay solenoid and the conventional quadrupoles have been in place for some time The MICE collaboration will demonstrate ionization cooling and subsequent reacceleration by 2017 and will use Lithium Hydride and liquid Hydrogen absorbers in two separate experiments The acceleration will be provided by two 201MHz cavities This will provide an understanding of muon cooling for use in a neutrino factory or for a proposed muon collider which will be multi TeV - “Higgs factory”

Acknowledgements STFC Rutherford Appleton Laboratory Elwyn Baynham Victoria Bayliss Roy Preece Stephen Watson Mike Courthold Mark Tucker STFC Daresbury Laboratory Stephen Griffiths Ian Mullacrane Chris White Trevor Hartnett Oxford University John Cobb Wing Lau Lawrence Berkeley National Laboratory Steven Virostek Michael Green Imperial College London Victoria Blackmore Fermilab Durga Rajaram

END