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MuCool Program

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Title: MuCool Program


1
MuCool Program
  • Muon Cooling RD
  • Alan Bross

2
MuCool
  • Mission
  • Design, prototype and test all cooling channel
    components
  • 201 MHz RF Cavities, LH2 absorbers, SC solenoids
  • Support MICE (cooling demonstration experiment)
  • Perform high beam-power engineering test of
    cooling section components
  • Consists of 10 institutions from the US, UK and
    Japan

RF Development ANL Cockcroft Institute Fermilab II
T JLAB LBNL Mississippi
Absorber RD Fermilab IIT KEK NIU Mississippi Osak
a
Solenoids LBNL Mississippi
3
MuCool Test Area
  • Facility to test all components of cooling
    channel (not a test of ionization cooling)
  • At high proton beam power
  • Designed to accommodate full Linac Proton Beam
    Power
  • 1.6 X 1013 p/pulse _at_15 Hz
  • 2.4 X 1014 p/s
  • 600 W into 35 cm LH2 absorber _at_ 400 MeV
  • RF power from Linac (201 and 805 MHz test stands)
  • Waveguides pipe power to MTA

4
MTA Hall
5
MTA
  • The MTA is the focus of our Activities
  • RF testing (805 and 201 MHz)
  • High pressure H2 gas-filled RF
  • LH2 Absorber tests
  • High Intensity Proton Beam
  • Will start with low intensity

6
MTA Hall Instrumentation
Chipmunk
Plastic Scintillator
805
CsI
201
Magnet
7
RF Cavity R and D
  • ANL/FNAL/IIT/LBNL/UMiss

8
RF RD Program
  • Basic Questions
  • Can we do anything to make MICE work better?
  • How does magnetic field affect rf cavities
  • What materials and material properties are
    desirable?
  • What surface modification is possible?
  • NF and Muon Colliders also require SCRF, Can we
    optimize this?
  • Accomplishments
  • Better understanding of conditioning with
    magnetic field in 805 cavity.
  • Full gradient operation of 201 MHz cavity in
    solenoid fringe field
  • Installation of Be windows and button test
    assembly.
  • Better modeling of breakdown limits.
  • Involvement with SCRF and material science
    community

9
RF RD Program II
  • Major papers
  • X ray Spectra, Nucl. Instrum. Meth. Phys. Rev. A.
    472, 600 (2001)
  • http//www-mucool.fnal.gov/mcnotes/public/pdf/muc0
    139/muc0139.pdf
  • Measurements of x-rays from a single cell cavity
  • Open Cell Cavity, Phys. Rev. STAB 6, 072001
    (2003)
  • http//link.aps.org/doi/10.1103/PhysRevSTAB.6.0720
    01
  • Measurements of 6 cell cavity, dark current
    measurements, w/wo B fields, comp. with other
    cavities, tensile stress
  • Cluster emission, Phys. Rev. STAB 7, 122001
    (2004)
  • http//link.aps.org/doi/10.1103/PhysRevSTAB.7.1220
    01
  • Emission of clusters, thermal and field
    dependence,
  • Breakdown mechanics, Nucl. Instrum. and Meth A
    537, 510, (2005)
  • http//www-mucool.fnal.gov/mcnotes/public/pdf/muc0
    286/muc0286.pdf
  • General theory of tensile stress triggered
    breakdown
  • Magnetic fields, Phys. Rev. STAB 8, 072001 (2005)
  • http//link.aps.org/doi/10.1103/PhysRevSTAB.8.0720
    01
  • Measurements with 805 MHz pillbox, measurement of
    s2(b)
  • Surface damage, Phys. Rev. STAB 9, 062001 (2006)
  • http//link.aps.org/doi/10.1103/PhysRevSTAB.9.0620
    01
  • Relationship between surface damage and maximum
    operating fields.

10
Fundamental Focus Of RF RD
  • Study the limits on Accelerating Gradient in NCRF
    cavities in magnetic field
  • We believe that the behavior of RF systems in
    general can be accurately described (predicted)
    by universal curves
  • This applies to all accelerating structures

11
805 MHz
  • Data seem to follow universal curve
  • Max stable gradient degrades quickly with B field
  • Remeasured
  • Same results
  • Does not condition

Gradient in MV/m
Peak Magnetic Field in T at the Window
12
805 MHz Imaging
13
Next 805 MHz study - Buttons
  • Button test
  • Evaluate various materials and coatings
  • Quick Change over

14
Field Profile Button Cell
  • Button Insert has replaced one of the curved Be
    windows
  • Second Be window still installed facing out

15
First Set of Button Data TiN Coated Cu
16
TiN Coated Cu After Running
17
TiN Coated Cu After Running II
18
2nd Round of Button Tests
19
Simplified layout of the Vertical mounting
To Existing Waveguide
New vertical Mechanical support holder
Current position in the magnet
The cavity will be moved into magnet about
half-in and half-out.
Anchored to base
20
High Pressure H2 Filled Cavity WorkMuons Inc
  • High Pressure Test Cell
  • Study breakdown properties of materials in H2
  • Operation in B field
  • No degradation in M.S.G. up to 3.5T

21
RF RD 201 MHz Cavity Design
  • The 201 MHz Cavity 19 MV/m Gradient Achieved
  • In low (few hundred G) B field. Still no
    breakdown. Limited by available power

22
Opening the 201
  • Shiniest Copper I have ever seen Jim Norem
    circa 2007

23
201 MHz Curved Be Window before Installation
24
201 MHz Cavity Operation in B Field
  • Initial 201 MHz operation in B Field
  • Limited to few hundred Gauss
  • Using Fringe Field of 4T magnet (in blue)

25
  • Need Coupling Coil (2.5T) MICE design
  • Shown in green schematically
  • THIS IS A CRUCIAL TEST FOR MICE AND FOR NF MC
    in general
  • High Gradient RF operation in a magnetic field

26
MICE Coupling Coil for MTA
Pro/E drawing by C.S.Liu
27
Absorber R and D
  • IIT/KEK/NIU/Osaka/UMiss

28
Absorber Design Issues
  • 2D Transverse Cooling
  • and
  • Figure of merit MLRdEm/ds
  • M2 (4D cooling) for different absorbers

H2 is clearly Best - Neglecting Engineering
Issues Windows, Safety
29
Absorber Engineering
  • Two LH2 absorber designs are being studied
  • Handle the power load differently

Forced-Convection-cooled. Has internal
heat exchanger (LHe) and heater KEK System
Forced-Flow with external cooling loop
30
Convective Absorber Activities
  • First Round of studies of the KEK absorber
    performed in the MTA
  • GHe used to input power

31
Convective Absorber Activities II
32
Convective Absorber Activities
  • KEK Convector Absorber upgrades
  • Electrical Heater
  • New Temperature sensors
  • LH liquid level sensor
  • Have now been installed and system has been
    tested
  • Ready for LH2 run
  • After safety approval

Absorber Body being modified in Lab 6 at Fermilab
33
LiH Test Program
  • Produce encapsulating cast (not pressed) samples
  • Small disks (5-10 cm)
  • Test casting procedures
  • Examine mechanical properties
  • Destructive tests for voids
  • Large disk (30 cm) for detailed thermal
    conductivity studies
  • External Cooling Internal Heating
  • Potential absorber for MICE Phase I
  • Non-instrumented, no cooling

NOT
34
Engineering Design for Large Disks
3/8 nut
Handle
Cap for copper tube
Guiding lid
High temp glass ceramic
High temp low k gasket
1 copper tube
High temp low k gasket
12 SS 316L ring
High temp glass ceramic
Thermocouples K (900C)
Supports
SS base plate attached to vibrator
Thermocouple holders
35
Production of LiH Disks
  • Only 1 vendor was found that would cast LiH
  • After some reflection (and some input from
    Chemists from Argonne Lab), the vendor decided
    casting LiH was too dangerous (production of H2
    gas)
  • Made a Third Attempt to work with Y12 (Oakridge)
  • Found the engineer in charge of their LiH work
    and he suggested that that press (Hot (150C,
    Isostatic (30,000 psi) a loaf and machine parts
    to our specification from the loaf
  • They have achieved 98 theoretical density using
    this technique
  • They are doing RD on casting LiH for their
    internal programs, but do not recommend it for
    our application.
  • It is very tricky due to the high temperature
    (700C ) and the large (30) shrinkage on cooling
  • We are in the process of setting up a contract
    with them to make a disk for temperature studies
    and 1 or 2 disks for MICE
  • Note The Li in their LiH is 6Li
  • For the mass we will receive, our parts will be
    considered Nuclear Material
  • PAPERWORK!!!

36
Machined Lithium Hydride Disc
  • Produced by Hot Isostatic Pressing
  • Produced using existing mold design provided by
    vendor
  • Tested by chemistry
  • X-Rayed by Radiography to ensure no voids
  • Machined to size as specified by FermiLab
  • Dimensional inspected against final customer
    supplied specification
  • Packaged in drum type container
  • Shipped by Fed-X

12 Blind holes for housing thermo-couples
37
1 thick foam board
1 copper tube with heater inside
High temp glass ceramic
The Set Up of the Thermal Test
High temp low k gasket
Machined LiH disc
12 dia steel ring
Thermocouples
Flexible cooling tube
Stainless steel base structure
38
The Set Up Ready for the Thermal Test
39
MuCool Phase II
  • Cryo-Infrastructure Installation
  • Beam Line Installation

40
MTA Cryo-Infrastructure
  • We are making good progress with completion of
    the cryo-plant and transfer-line system.
  • Transfer line system parts complete
  • Our goal is to install/commission the system this
    FY (well our goal was to install last FY)
  • Before the shutdown (August) in we can start by
    June
  • We define the beginning of the window to be when
    the cryo-plant is up and running (producing LHe)
  • After the shutdown otherwise
  • Our current operating costs (LHe) for the MTA
    magnet are 3-5k/week
  • Fermilab is providing 100k of support for MTA
    operations
  • Will allow us to run the magnet off LHe dewars
    for the remainder of FY07 if required

41
Existing Dewar-Fed Cryogen System
  • All of this is removed
  • New (simpler) shield wall
  • Will allow for easier pit access to hall
  • More shielding needed for beam operations in MTA
    Hall

42
MTA Refrigerator RoomArtists Conception
43
Storage Area
GHe, LN2 Storage Heat Exch.
44
Compressor Room
45
Refrigerator Room
46
Transfer Line System
47
Transfer Line System
Valve Box Piping
48
Completed Valve Box
49
Refrig Room Valve Can
50
Xfer Line
51
MTA Beam Line Group
52
MTA Beam Line
  • 400 MeV beamline for the MTA has been designed
  • Under Craig Moore/Carol Johnstone
  • External Beams Department
  • Engineering Design mature
  • Cost
  • Safety Analysis
  • Linac Area and Beamline
  • Shielding Assessment for MTA
  • First Phase will be low-intensity
  • Funded by Fermilab NFMCC
  • Installation group now formed
  • F. Garcia (Proton source group)

MTA
53
MTA Beam Line
54
First Beam Experiments
  • Currently 5T magnet and 201 cavity on floor
    (below beam ht.)
  • First experiments will pitch beam down to center
    of magnet
  • Allows for early tests of gas filled cavity
    operation in intense beam
  • Very-low integrated intensity
  • Few full-intensity linac pulses

55
  • Beam Line commissioning begins in early 2008,
    first tests with beam in June
  • Designed to accommodate full Linac Beam
  • 1.6 X 1013 p/pulse _at_15 Hz
  • 2.4 X 1014 p/s
  • 600 W into 35 cm LH2 absorber _at_ 400 MeV
  • Will start at low intensity
  • Need Shielding upgrade (over-burden) for
    high-intensity

56
Phase II
  • Raise equipment to beam height
  • Install cryo-infrastructure
  • Valve box
  • Transfer lines
  • Weld system
  • Connect to cryo-plant
  • Expect 2-3 month duration with appropriate
    technical resources

57
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58
  • Addition of Coupling Coil (B field studies of 201
    operation) requires the 201 MHz cavity to be
    rotated 180 degree

59
MuCool Plans for the Coming Year
  • 805 MHz RF studies Buttons (with and without B
    field)
  • Materials tests
  • Surface treatment
  • E X B study
  • 201 MHz RF
  • Move cavity close to magnet and repeat studies _at_
    high (1T) B
  • Begin thermal and mechanical tests on HIP LiH
    absorber prototypes
  • Complete MTA cryo infrastructure installation and
    commission system
  • Commission Beam Line
  • First tests with Beam
  • Test of HP H2 RF test cell with beam
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