Muons, Inc. MANX Update: MANX Following MICE at RAL MICE cm 23 – January 14, 2008 Richard Sah.

Slides:



Advertisements
Similar presentations
12/20/ minutes on 11 projects 1 Muons, Inc. Grants and Proposals Rolland Johnson, Muons, Inc. Muons, Inc. Grants and Proposals Rolland Johnson,
Advertisements

Muons, Inc. 12/1/2009Dec 1-3, 2009 MCDW at BNL Cary Y. Yoshikawa 1 Use of a Quasi-Isochronous Helical Cooling Channel in the Front End of a Muon Collider.
12/5/2008NuMu Collaboration Friday Meeting 1 Status Report on MANX Proposal Draft Bob Abrams Muons, Inc.
Bunched-Beam Phase Rotation- Variation and 0ptimization David Neuffer, A. Poklonskiy Fermilab.
RF Bucket Area Introduction Intense muon beams have many potential applications, including neutrino factories and muon colliders. However, muons are produced.
MICE: The International Muon Ionization Cooling Experiment Diagnostic Systems Tracker Cherenkov Detector Time of Flight Counters Calorimeter Terry Hart.
July 28, 2004K. Yonehara, NuFact'04 Osaka1 High pressure RF cavities for muon beam cooling Katsuya Yonehara Illinois Institute of Technology NuFact04 in.
Rol Johnson 6/28/2005 MICE/MANX 1 MANX: a 6D Cooling Demonstration Experiment Rolland P. Johnson MANX: a 6D Cooling Demonstration Experiment Rolland P.
Helical Cooling Channel Simulation with ICOOL and G4BL K. Yonehara Muon collider meeting, Miami Dec. 13, 2004 Slide 1.
February 24, 2007MICE CM171 6D MANX A Muon Cooling Demonstration Experiment; How it might fit with MICE. Tom Roberts Muons, Inc.
Muons, Inc. AAC Feb. 4, 2009 V. Kashikhin 1 Fermilab AAC  V. Kashikhin for Superconducting Magnet Team Superconducting Helical Solenoids.
04/28/04MUTAC BNL1 Muons, Inc. Status: Six SBIR/STTR Muon Projects Rolland Johnson, April 28, 2004 HP HG GH2 RF –Ph II, w IIT, DK 6D Cooling on Helix –Ph.
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.
Feb 15, 2008S. Kahn -- RF in HCC Channel1 Examination of How to Put RF into the HCC Steve Kahn Katsuya Yonehara NFMCC Meeting Feb 15, 2008 Muons, Inc.
Fast TOF for Muon Cooling Experiments Robert Abrams Muons, inc.
Rol - Dec. 9, 2008 MC Design Workshop JLab 1 Low Emittance Muon Collider Development Rolland P. Johnson Muons, Inc. (
Institutional Logo Here Harold G. Kirk DOE Review of MAP (FNAL August 29-31, 2012)1 The Front End Harold Kirk Brookhaven National Lab August 30, 2012.
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.
Muons, Inc. AAC Feb M. A. C. Cummings 1 Uses of the HCC Mary Anne Cummings February 4, 2009 Fermilab AAC.
Mar 19, 2008 S. Kahn -- RF in HCC Channel 1 Examination of How to Put RF into the HCC Steve Kahn NFMCC Meeting Mar 19, 2008.
Status of the Muon Ionization Cooling Experiment (MICE) Yagmur Torun Illinois Institute of Technology April 1, 2013.
The 2010 NFMCC Collaboration Meeting University of Mississippi, January 13-16, Update on Parametric-resonance Ionization Cooling (PIC) V.S. Morozov.
Particle Production in the MICE Beam Line Particle Accelerator Conference, May 2009, Vancouver, Canada Particle Production in the MICE Beam Line Jean-Sebastien.
Considerations on Interaction Region design for Muon Collider Muon Collider Design Workshop JLab, December 8-12, 2008 Guimei Wang, Muons,Inc., /ODU/JLab.
Rol - Oct 23, 2007 Cosener's NFMC TW 1 Helical Cooling Channels (and related items) Rolland P. Johnson Muons, Inc. Please visit "Papers and Reports" and.
Rol - Feb. 3, 2009 AAC Meeting 1 MANX- Toward Bright Muon Beams for Colliders, Neutrino Factories, and Muon Physics Rolland P. Johnson Muons, Inc. (
Rol - Feb. 3, 2009 AAC Meeting 1 MANX- Toward Bright Muon Beams for Colliders, Neutrino Factories, and Muon Physics Rolland P. Johnson Muons, Inc. (
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
Thomas Jefferson National Accelerator Facility Page 1 Muons, Inc. Epicyclic Helical Channels for Parametric-resonance Ionization Cooling Andrei Afanasev,
Rol - 8/8/2007 AAC MANX Intro 1 Introduction: Low Emittance Muon Collider, New 6D Cooling Ideas, and MANX Rol Johnson Muons, Inc.
Rol Johnson 7/22/2005 JLab Seminar 1 Recent Innovations in Muon Beam Cooling and Prospects for Muon Colliders and Neutrino Factories Rolland P. Johnson.
K. McDonald NFMCC Collaboration Meeting Jan 14, The Capture Solenoid as an Emittance-Reducing Element K. McDonald Princeton U. (Jan. 14, 2010)
Thomas Jefferson National Accelerator Facility Page 1 Muons, Inc. HCC theory Yaroslav Derbenev, JLab Rolland P. Johnson, Muons, Inc Andrei Afanasev, Hampton.
1 EPIC SIMULATIONS V.S. Morozov, Y.S. Derbenev Thomas Jefferson National Accelerator Facility A. Afanasev Hampton University R.P. Johnson Muons, Inc. Operated.
V.Balbekov, 12/09/08 HCC simulation with wedge absorbers V. Balbekov, Fermilab Muon Collider Design Workshop December 8-12, 2008 JeffersonLab, Newport.
J. Pasternak First Ideas on the Design of the Beam Transport and the Final Focus for the NF Target J. Pasternak, Imperial College London / RAL STFC ,
Rol - 8/3/2010 Slava Symposium 1 The Entrepreneurial Slava or why the next energy frontier/ lepton collider will be  +  - Muons, Inc. Rolland Johnson,
Rol Johnson 6/21/2005 NuFact05 WG3 1 Comparing Neutrino Factory and Muon Collider Beam Cooling Requirements Rolland P. Johnson Comparing Neutrino Factory.
-Factory Front End Phase Rotation Gas-filled rf David Neuffer Fermilab Muons, Inc.
MICE at STFC-RAL The International Muon Ionization Cooling Experiment -- Design, engineer and build a section of cooling channel capable of giving the.
MANX at MTA Andreas Jansson Fermilab. 2/14/2007LEMC Workshop, February 12-16, 2007A. Jansson 2 Foreseen MCTF Experimental R&D Low energy proton beam to.
Updated 04/26/05MUTAC1 SBIR/STTR Beam Cooling Projects BNL, FNAL, IIT, Jlab, Muons, Inc. Rolland Johnson, updated April 26, 2005 GH 2 RF cavitiesIIT, Kaplan.
Bright muon sources Pavel Snopok Illinois Institute of Technology and Fermilab August 29, 2014.
MICE: The International Muon Ionisation Cooling Experiment MOPLT106 Abstract The provision of intense stored muon beams would allow the properties of neutrinos.
Rol - Jan 28, 2011 MEIC Workshop 1 A Business Inspired by Muon Colliders (Can it contribute to electron-ion colliders?) Rolland P. Johnson Muons, Inc.
Timing measurements at the MICE experiment – 1 The analysis of timing measurements at the Muon Ionization Cooling Experiment Mark Rayner The University.
Institutional Logo Here July 11, 2012 Muon Accelerator Program Advisory Committee Review (FNAL July 11-13, 2012)1 The Front End.
Simulating the RFOFO Ring with Geant Amit Klier University of California, Riverside Muon Collaboration Meeting Riverside, January 2004.
Ionization Cooling for a     Collider David Neuffer Fermilab 7/15/06.
Lecture 4 Longitudinal Dynamics I Professor Emmanuel Tsesmelis Directorate Office, CERN Department of Physics, University of Oxford ACAS School for Accelerator.
MANX and Muon collider progress Katsuya Yonehara Fermi National Accelerator Lab DPF2006, Honolulu, Hawai’i October 30 th, 2006.
Monte Carlo simulation of the particle identification (PID) system of the Muon Ionization Cooling Experiment (MICE) Mice is mainly an accelerator physics.
1 Front End – present status David Neuffer December 4, 2014.
Jun 13, 2008 Synergy ‘08 MANX, a 6-D Muon Cooling Experiment MACC Muons, Inc.
August 8, 2007 AAC'07 K. Yonehara 1 Cooling simulations for Muon Collider and 6DMANX Katsuya Yonehara Fermilab APC MCTF.
Muons, Inc. Feb Yonehara-AAC AAC Meeting Design of the MANX experiment Katsuya Yonehara Fermilab APC February 4, 2009.
MICE. Outline Experimental methods and goals Beam line Diagnostics – In HEP parlance – the detectors Magnet system 2MICE Optics Review January 14, 2016.
Research and development toward a future Muon Collider Katsuya Yonehara Accelerator Physics Center, Fermilab On behalf of Muon Accelerator Program Draft.
MICE. Outline Experimental methods and goals Beam line Diagnostics – In HEP parlance – the detectors Magnet system 2MICE Optics Review January 14, 2016.
Uses of the HCC Mary Anne Cummings February 4, 2009 Fermilab AAC
Rolland Johnson, Muons, Inc.
Parametric Resonance Ionization Cooling of Muons
m MANX- Toward Bright Muon Beams
HCC theory Yaroslav Derbenev, JLab Rolland P. Johnson, Muons, Inc
Superconducting Helical Solenoids
M Muons, Inc. Comparing Neutrino Factory and Muon Collider Beam Cooling Requirements Rolland P. Johnson Neutrino Factories need a large muon flux to produce.
Design of the MANX experiment
K. Tilley, ISIS, Rutherford Appleton Laboratory, UK Introduction
The Detector System of the MICE Experiment
Uses of the HCC Mary Anne Cummings February 4, 2009 Fermilab AAC
Presentation transcript:

Muons, Inc. MANX Update: MANX Following MICE at RAL MICE cm 23 – January 14, 2008 Richard Sah

Muons, Inc. 2 Richard Sah – MICE cm23 January 14, 2009 Outline MANX Concept MANX Concept Helical Cooling Channels (6-D Cooling) Helical Cooling Channels (6-D Cooling) MANX Following MICE at RAL MANX Following MICE at RAL

Muons, Inc. 3 Richard Sah – MICE cm23 January 14, 2009 MANX Concept Muon Collider and Neutrino Factory Ionization Cooling Experiment (MANX) Muon Collider and Neutrino Factory Ionization Cooling Experiment (MANX) Construction of a Helical Solenoid (HS) and its installation at RAL as part of MICE. This HS magnet is very similar to that used in simulations of the mu2e experimental upgrade for the Project-X era at Fermilab Construction of a Helical Solenoid (HS) and its installation at RAL as part of MICE. This HS magnet is very similar to that used in simulations of the mu2e experimental upgrade for the Project-X era at Fermilab Goals and Organization Goals and Organization Test of momentum-dependent Helical Cooling Channel (HCC), applicable to muon colliders, neutrino factories, and stopping muon beams Test of momentum-dependent Helical Cooling Channel (HCC), applicable to muon colliders, neutrino factories, and stopping muon beams Proposal to organize MANX as a joint Fermilab-RAL project Proposal to organize MANX as a joint Fermilab-RAL project Fermilab responsible for magnet and detector upgrades Fermilab responsible for magnet and detector upgrades RAL provides the MICE beam line, where much of the MICE apparatus can be reused RAL provides the MICE beam line, where much of the MICE apparatus can be reused

Muons, Inc. 4 Richard Sah – MICE cm23 January 14, 2009 Key MANX features Key MANX features Will Test: Will Test: Theory of Helical Cooling Channel (HCC) Theory of Helical Cooling Channel (HCC) p-dependent HCC with continuous absorber p-dependent HCC with continuous absorber Helical Solenoid Magnet (HS) and absorber similar to that required for upgrade to mu2e experiment Helical Solenoid Magnet (HS) and absorber similar to that required for upgrade to mu2e experiment Simulation programs (G4BL, ICOOL) Simulation programs (G4BL, ICOOL) Minimizes costs and time Minimizes costs and time no RF, uses normalized emittance, ~5 m LHe E absorber no RF, uses normalized emittance, ~5 m LHe E absorber RF is developed in parallel with new concepts RF is developed in parallel with new concepts builds on MICE, adds 6-d capability, ~ps detectors builds on MICE, adds 6-d capability, ~ps detectors

Muons, Inc. 5 Richard Sah – MICE cm23 January 14, 2009 Outline: HCC In recent years, the concept of Helical Cooling Channels has been invented and developed for 6-D muon-beam cooling In recent years, the concept of Helical Cooling Channels has been invented and developed for 6-D muon-beam cooling Ionization Cooling Ionization Cooling Transverse Emittance IC Transverse Emittance IC Wedges or Continuous Energy Absorbers Wedges or Continuous Energy Absorbers Helical Cooling Channels (HCC) Helical Cooling Channels (HCC)

6 6 Each particle loses momentum by ionizing a low-Z absorber Only the longitudinal momentum is restored by RF cavities The angular divergence is reduced until limited by multiple scattering Successive applications of this principle with clever variations leads to small emittances for many applications Early work: Budker, Ado & Balbekov, Skrinsky & Parkhomchuk, Neuffer Principle of Ionization Cooling Muons, Inc.

7 Richard Sah – MICE cm23 January 14, 2009 Transverse Emittance IC The equation describing the rate of cooling is a balance between cooling (first term) and heating (second term): The equation describing the rate of cooling is a balance between cooling (first term) and heating (second term): Here  n is the normalized emittance, E µ is the muon energy in GeV, dE µ /ds and X 0 are the energy loss and radiation length of the absorber medium,   is the transverse beta-function of the magnetic channel, and  is the particle velocity. Here  n is the normalized emittance, E µ is the muon energy in GeV, dE µ /ds and X 0 are the energy loss and radiation length of the absorber medium,   is the transverse beta-function of the magnetic channel, and  is the particle velocity. Bethe-BlochMoliere (with low Z mods)

Muons, Inc. 8 Richard Sah – MICE cm23 January 14, 2009 Ionization Cooling is only transverse. To get 6D cooling, emittance exchange between transverse and longitudinal coordinates is needed. THIS RH CONCEPTUAL PICTURE BE REALIZED? A MANX GOAL! Wedges or Continuous Energy Absorber for Emittance Exchange and 6d Cooling

Muons, Inc. 9 Richard Sah – MICE cm23 January 14, 2009 Helical Cooling Channel First simulations showed factor of ~150,000 reduction in 6d emittance in less than 100 m of HCC. First simulations showed factor of ~150,000 reduction in 6d emittance in less than 100 m of HCC. ~40,000 microns normalized transverse acceptance ~40,000 microns normalized transverse acceptance Used 200 MHz H2-pressurized cavities inside magnet coils. (absorber and RF occupy same space) Used 200 MHz H2-pressurized cavities inside magnet coils. (absorber and RF occupy same space) Engineering Implementation requires creativity Engineering Implementation requires creativity Coils outside of such large RF Cavities are difficult. Solutions? Coils outside of such large RF Cavities are difficult. Solutions? bigger coils: Helical Solenoid with/without correction coils bigger coils: Helical Solenoid with/without correction coils smaller cavities: 1) dielectric-loaded or 2) traveling wave solutions smaller cavities: 1) dielectric-loaded or 2) traveling wave solutions smaller pitch angle (weaker helical dipole) eases field at conductor smaller pitch angle (weaker helical dipole) eases field at conductor H2-Pressurized RF cavities are undeveloped/unproven H2-Pressurized RF cavities are undeveloped/unproven Max RF gradient shown to be insensitive to external B field. Max RF gradient shown to be insensitive to external B field. MTA proton beam tests soon. (SF6 dopant calcs/tests encouraging) MTA proton beam tests soon. (SF6 dopant calcs/tests encouraging)

Muons, Inc. 10 Richard Sah – MICE cm23 January 14, Dimensional Cooling in a Continuous Absorber Helical cooling channel (HCC) Helical cooling channel (HCC) Continuous absorber for emittance exchange Continuous absorber for emittance exchange Solenoidal, transverse helical dipole and quadrupole fields Solenoidal, transverse helical dipole and quadrupole fields Helical dipoles known from Siberian Snakes Helical dipoles known from Siberian Snakes z- and time-independent Hamiltonian z- and time-independent Hamiltonian Derbenev & Johnson, Theory of HCC, April/05 PRST-AB Derbenev & Johnson, Theory of HCC, April/05 PRST-AB

1111 Particle Motion in an HCC Magnet Blue: Beam envelope Red: Reference orbit Magnet Center Combined function magnet (invisible in this picture) Solenoid + Helical dipole + Helical Quadrupole Dispersive component makes longer path length for higher momentum particles and shorter path length for lower momentum particles. Opposing radial forces Transforming to the frame of the rotating helical dipole leads to a time and z – independent Hamiltonian b' added for stability and acceptance

12 Some Important Relationships 12 Hamiltonian Solution Equal cooling decrements Longitudinal cooling only ~Momentum slip factor ~ Muons, Inc.

1313 Two Different Designs of Helical Cooling Magnet Siberian snake type magnet Consists of 4 layers of helix dipole to produce tapered helical dipole fields. Coil diameter is 1.0 m. Maximum field is more than 10 T. Helical solenoid coil magnet Consists of 73 single coils (no tilt). Maximum field is 5 T Coil diameter is 0.5 m. Large bore channel (conventional) Small bore channel (helical solenoid) Great new innovation! Muons, Inc.

1414 HS for Cooling Demonstration Experiment Goals: cooling demonstration, HS technology development Features: SSC NbTi cable, B max ~6 T, coil ID ~0.5m, length ~10m

Muons, Inc. 15 Richard Sah – MICE cm23 January 14, 2009 Outline: MANX Following MICE at RAL What It Is What It Is Changes Required for MANX Changes Required for MANX Current Status of MANX Current Status of MANX Participating Institutions Participating Institutions Summary Summary

Muons, Inc. 16 Richard Sah – MICE cm23 January 14, 2009 MANX Following MICE at RAL

Muons, Inc. 17 Richard Sah – MICE cm23 January 14, 2009 MANX Following MICE The HS will be installed at the MICE beam line, where much of the MICE apparatus can be reused. The HS will be installed at the MICE beam line, where much of the MICE apparatus can be reused. However, changes will be required However, changes will be required Incident muon beam momentum increased to 350 MeV/c Incident muon beam momentum increased to 350 MeV/c MANX requires more precise longitudinal momentum resolution, for a MANX requires more precise longitudinal momentum resolution, for a 6-D cooling experiment, perhaps by TOF measurements MANX may need upgraded Cherenkov counters to identify muons and reject pions at 350 MeV/c MANX may need upgraded Cherenkov counters to identify muons and reject pions at 350 MeV/c Particle trajectories must be measured at a number of positions within the cooling channel, in order to test the theory of cooling within the HCC Particle trajectories must be measured at a number of positions within the cooling channel, in order to test the theory of cooling within the HCC There may be differences in triggering and in DAQ There may be differences in triggering and in DAQ Experimental layout must be reconfigured for the HCC, matching sections, and detectors Experimental layout must be reconfigured for the HCC, matching sections, and detectors

Muons, Inc. 18 Richard Sah – MICE cm23 January 14, 2009 Muons, Inc. Project History Underlined are explicitly related to HCC Underlined are explicitly related to HCC YearProject Expected Funds Research Partner High Pressure RF Cavity$600,000 IIT (Dan K.) Helical Cooling Channel$850,000Jlab (Slava D.) MANX demo experiment$ 95,000FNAL TD (Victor Y.) Phase Ionization Cooling$745,000Jlab (Slava D.) HTS Magnets$795,000FNAL TD (Victor Y.) Reverse Emittance Exch.$850,000Jlab (Slava D.) Capture, ph. rotation$850,000FNAL AD (Dave N.) G4BL Sim. Program$850,000 IIT (Dan K.) MANX 6D Cooling Demo $850,000FNAL TD (M. Lamm) Stopping Muon Beams$750,000FNAL APC (Chuck A.) HCC Magnets$750,000FNAL TD (Sasha Z.) Compact, Tunable RF$100,000FNAL AD (Milorad P.) Pulsed Quad RLAs$100,000Jlab (Alex B.) Fiber Optics for HTS$100,000FSU (Justin S.) RF Breakdown Studies$100,000LBNL (Derun L.) Rugged RF Windows$100,000Jlab (Bob Rimmer) H2-filled RF Cavities$100,000FNAL APC (Katsuya Y.) 2009Illinois matching $150,000DCEO (Hedin)

Muons, Inc. 19 Richard Sah – MICE cm23 January 14, 2009 HCC Magnets for MANX Prototype coils for MANX have been designed and modeled. Construction of a 4-coil assembly using SSC cable is complete. Tests in the TD vertical Dewar will start soon. Since the MANX matching sections are made of coils with varying offset, they are more expensive than the cooling region. Consequently the total magnet cost can be drastically reduced if the matching sections are not needed.

Muons, Inc. 20 Richard Sah – MICE cm23 January 14, 2009 HCC Magnets using HTS Beam cooling to reduce the size of a muon beam depends on the magnetic field strength. The Phase II proposal to develop this hybrid scheme has been approved. Here a hybrid magnet of Nb3Sn (green) and HTS (red) could provide up to 30 T in an HCC design.

Muons, Inc. 21 Richard Sah – MICE cm23 January 14, 2009 MANX as a Pre-cooler z = 0 m z = 3 m z = 6 m p (MeV/c) 10k POT Used LiH plate in this simulation Good transmission

Muons, Inc. 22 Richard Sah – MICE cm23 January 14, 2009 Simpler Option without Matching Sections LHe or LH2 region Matching sections Requires transverse displacement of downstream spectrometer Magnet ~$10M Magnet < $5M

Muons, Inc. 23 Richard Sah – MICE cm23 January 14, 2009 Discussions with MICE Collaboration Rolland Johnson presented the idea of “MANX Following MICE at RAL” to the MICE Collaboration (October 20, 2008, at RAL) Rolland Johnson presented the idea of “MANX Following MICE at RAL” to the MICE Collaboration (October 20, 2008, at RAL) A MICE Collaboration Committee was formed to investigate this concept A MICE Collaboration Committee was formed to investigate this concept Questions were posed by John Cobb Questions were posed by John Cobb Answers have been provided by Muons, Inc. Answers have been provided by Muons, Inc. Feb 09 presentation to FNAL AAC has been scheduled Feb 09 presentation to FNAL AAC has been scheduled A 55-page proposal has been prepared A 55-page proposal has been prepared Will request support from FNAL for MANX at MICE ($5-10M magnet) Will request support from FNAL for MANX at MICE ($5-10M magnet) An expression of interest from the MICE collaboration would be very welcome! An expression of interest from the MICE collaboration would be very welcome! We invite HIT to become seriously involved in the HS for MANX. We invite HIT to become seriously involved in the HS for MANX.

Muons, Inc. 24 Richard Sah – MICE cm23 January 14, 2009 Participating Institutions Muons, Inc. Fermi National Accelerator Laboratory Thomas Jefferson National Accelerator Facility University of Chicago University of California at Riverside Illinois Institute of Technology Northern Illinois University

Muons, Inc. 25 Richard Sah – MICE cm23 January 14, 2009 Summary: MANX Will Test: Will Test: Theory of Helical Cooling Channel (HCC) Theory of Helical Cooling Channel (HCC) p-dependent HCC with continuous absorber p-dependent HCC with continuous absorber Helical Solenoid Magnet (HS) and absorber similar to that required for upgrade to mu2e experiment Helical Solenoid Magnet (HS) and absorber similar to that required for upgrade to mu2e experiment Simulation programs (G4BL, ICOOL) Simulation programs (G4BL, ICOOL) Minimizes costs and time Minimizes costs and time no RF, uses normalized emittance, ~5 m LHe E absorber no RF, uses normalized emittance, ~5 m LHe E absorber RF is developed in parallel with new concepts RF is developed in parallel with new concepts builds on MICE, adds 6-D capability, ~ps detectors builds on MICE, adds 6-D capability, ~ps detectors