The Spallation Neutron Source: A Powerful Tool for Materials Research PowerPoint PPT Presentation

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Title: The Spallation Neutron Source: A Powerful Tool for Materials Research


1
The Spallation Neutron SourceA Powerful Tool
for Materials Research
PAC2001
  • T. E. Mason
  • Associate Laboratory Director for the SNS

June 18, 2001
2000-0xxxx/vlb
2
Structure Determines Properties
  • 3 forms of Carbon - very different materials

Graphite
Diamond
Buckyballs
3
Knowledge of structure and dynamics leads to new
materials
  • Superconductors or organic ferromagnets

4
Scientific justification for SNS
  • Neutrons provide unique insight into materials at
    the atomic level
  • see light atoms in biomaterials and polymers
  • study magnetic properties and atomic motion
  • measure stress in engineering components
  • Neutron scattering was developed in the US but we
    now have a serious shortage of facilities and
    they are not best in the world
  • State-of-the-art neutron source has been an
    urgent priority for 15 years
  • The SNS will be world leading and help restore US
    leadership

5

Neutrons and Neutron Sources
  • The neutron was discovered in 1932 by Chadwick
  • Coherent neutron diffraction (Bragg scattering by
    crystal lattice planes) was first demonstrated in
    1936 by Mitchel Powers and Halban Preiswerk
    as an exercise in wave mechanics
  • The possibility of using the scattering of
    neutrons as a probe of materials developed with
    the availability of copious quantities of slow
    neutrons from reactors after 1945. Fermi's group
    used Bragg scattering to measure nuclear
    cross-sections

98-6245 uc/vlb
6
Neutrons and Neutron Sources
  • A reactor moderates the neutrons produced in the
    fission chain reaction resulting in a Maxwellian
    energy distribution peaked at T (300K).

98-6243 uc/rfg
7

Neutrons and Neutron Sources
  • The application of slow neutron scattering to the
    study of condensed matter had its birth in the
    work of Wollan and Shull (1948) on neutron powder
    diffraction
  • The neutron is a weakly interacting,
    non-perturbing probe with simple, well-understood
    coupling to atoms and spins
  • The scattering experiment tells you about the
    sample not the probe

98-6244 uc/rfg
8

Neutrons and Neutron Sources
  • You can easily work in extreme sample
    environments H,T,P,...) e.g.4He cryostat (Shull
    Wollan) and penetrate into dense samples
  • The magnetic and nuclear cross-sections are
    comparable, nuclear cross-sections are similar
    across the periodic table
  • Sensitivity to a wide a range of properties, both
    magnetic and structural

98-6242 uc/rfg
9
Development of Neutron Science Facilities
97-3924E uc/djr
10
Neutrons Where?
  • Fission
  • n 235U n n fragments
  • moderated by available
  • D2O (H2O) to
  • E T (Maxwellian)

Sustain chain reaction
200 MeV/n
98-6239 uc/vlb
11
Types of Neutron Sources
  • Reactor e.g., ILL, France
  • 1.5x1015 n/cm2/s2 (recently underwent major
    refurbishment)
  • Advantages
  • high time averaged flux
  • mature technology (source instruments)
  • very good for cold neutrons
  • Drawbacks
  • licensing (cost/politics)
  • no time structure

98-6237 uc/rra
12
The Institut Laue-Langevin, Grenoble
2000-05269 uc/arb
13
Neutrons Where?
  • Spallation
  • p heavy nucleus 20 n fragments
  • 1GeV e.g. W, Pb, U
  • flux
  • DR3 Risf 2 x 1014 n/cm2/s
  • ILL Grenoble 1.5 x 1015 n/cm2/s
  • ISIS average 2 x 1013 n/cm2/s
  • 8 x 1015 n/cm2/s

23 MeV/n
98-6240 uc/vlb
14
Spallation-Evaporation Production of Neutrons
15
Types of Neutron Sources
  • Pulsed spallation source e.g., ISIS, LANSCE
  • 200 µA, 0.8 GeV, 160 kW
  • 2x1013 n/cm2/s2 average flux
  • 8x1015 n/cm2/s2 peak flux
  • Advantages
  • high peak flux
  • advantageous time structure for many applications
  • accelerator based politics simpler than
    reactors
  • technology rapidly evolving
  • Disadvantages
  • low time averaged flux
  • not all application exploit time structure
  • rapidly evolving technology

98-6235 uc/rra
16
ISIS Instruments
2000-05273 uc/arb
17
The Spallation Neutron Source
  • The SNS will begin operation in 2006
  • At 2 MW it will be 12x ISIS, the worlds leading
    pulsed spallation source
  • The peak thermal neutron flux will be 50-100x
    ILL
  • SNS will be the worlds leading facility for
    neutron scattering
  • It will be a short drive from HFIR, a reactor
    source with a flux comparable to the ILL

18
Spallation Neutron Source
  • Worlds largest civilian science project, 1.4
    Billion TPC
  • Will attract 1000-2000 users annually
  • University vs. industry users dominate
    (four-to-one)

01-02462/arb
19
Project Status
  • The FY 2002 request was 291M
  • The project now enjoys solid congressional
    support
  • Overall project design is 56 complete
  • Overall the project is 21.8 complete (through
    March 01) and within budget and schedule
    constraints
  • 1.4B and June 2006 completion
  • Initial safety documentation is now in place both
    for accelerator and instruments (PSAD) and target
    (PSAR)
  • There is good progress on all of the technical
    components front end, superconducting linac,
    ring, target, instruments
  • We have excellent ESH performance

20
Construction Progress
  • Completed two major access roads
  • Excavated over 1.4 million cubic yards during
    site preparation
  • Completed retention pond
  • Completed Linac tunnel excavation
  • Front End and Linac Tunnel concrete installation
    under way!
  • Completed installation of three temporary
    electrical distribution centers
  • Completed Target Building deep foundation
    installation

21
Inner plug assembly optimized for performance
Supercritical H2 Moderator decoupled poisoned
Supercritical H2 Moderator coupled
Beryllium Reflector
Lead Reflector
Proton Beam
Ambient Moderator decoupled poisoned
Supercritical H2 Moderator coupled
22
Instrument Systems Summary
  • Build best-in-class neutron scattering
    instruments to deliver maximum benefit from SNS
    performance characteristics
  • Develop shared designs for common components to
    be used by these instruments and future
    instruments
  • Carry out RD to drive the design of innovative
    instruments for the project and beyond
  • Instruments are being selected in consultation
    with the user community, Instrument Oversight
    Committee (now EFAC)

2000-03448/arb
23
SNS will be a USER facility
  • User input into the SNS instrument suite
  • Instrument Oversight Committee Workshops
  • Support (technical, scientific, logistical) for
    users carrying out experiments
  • Peer reviewed proposal system
  • 1000-2000 users per year from academia,
    government, and industry
  • Flexible instrument strategy that supports both
    general user access and dedicated access for
    expert instrument teams that contribute to
    construction and operation of instruments

24
Current Instrument Concepts
  • Nine instruments have been approved. (boldface
    funded)
  • High-resolution backscattering spectrometer
  • Magnetism reflectometer
  • Liquids reflectometer
  • Engineering materials diffractometer
  • Extended Q-range small-angle diffractometer
  • 6m chopper spectrometer
  • Third generation powder diffractometer
  • Inelastic spectrometer with 10-100 microvolt
    resolution
  • Disordered materials diffractometer
  • High pressure diffractometer
  • Concepts are being developed for additional
    instruments.
  • 2.5 m chopper spectrometer
  • High-speed single-crystal diffractometer
  • Spin echo
  • Fundamental neutron physics

25
Instruments in Instrument Hall
26
Melittin in Alkanethiol/Phospholipid Hybrid
Bilayer Membranes - NIST
27
Melittin in Alkanethiol/Phospholipid Hybrid
Bilayer Membranes - NIST
28
Reflectometry
  • In addition to providing a unique probe for
    magnetic surfaces and multi-layers polarized
    neutrons permit direct inversion to obtain the
    scattering length density profile - no phase
    problem
  • a magnetic reference layer buried in the
    substrate can have magnetization wrt neutron
    polarization varied
  • for a weak absorbtion probe (valid for the
    neutron) three known references lead to unique
    solution
  • drawback is the price paid in sensitivity for
    polarized beam
  • Off-specular reflection for in-plane structure

29
Reflectometers
  • 2 reflectometers sharing a single beamport
  • Requires new multi-channel shutters in the target
    station
  • Allows for both vertical sample (magnetism) and
    horizontal sample (liquids) studies
  • Novel beam bender optics allows multiplexing and
    reduces background
  • Reflectivities lt10-9, 10-50 times faster than any
    existing instrument

2000-03451/arb
30
Both Reflectometers w/o Shielding
31
VULCAN Is a Compound Instrument Designed to
Tackle Engineering Problems
  • Rapid volumetric (3D) mapping with a sampling
    volume of 1 mm3 and a measurement time of minutes
  • Very high spatial resolution (0.1 mm) in one
    direction with a measurement time of minutes
  • 20 well defined reflections for in-situ loading
    studies
  • Ability to study kinetic behaviors in sub second
  • Simultaneous SANS measurements
  • Ancillary equipment such as furnace and load
    frame will be an integrated part of the
    instrument
  • 30x SMARTS at Los Alamos

32
cAMP-Dependent Protein Kinase (PKA) Combining
Neutrons with X-rays
  • PKA catalyzes a variety of cellular activities,
    ranging from gene induction to color change in
    pigment cells.
  • PKA serves as the prototype for a class of
    enzymes which catalyzes protein phosphorylation,
    the major mechanism of cellular regulation.
  • The combination of neutron studies and x-ray
    structures of PKA subunits has provided insights
    into the quaternary structure of PKA, which is
    key to the understanding of PKA function.

33
SNS SANS
  • Extended Q-Range 0.001-12 Å-1
  • Moderate resolution
  • Performance 3-5 x D22 (ILL) HFIR, 30-100 x
    ISIS

34
Q-Coverage
Huey Huang Rice University
3rd Frame
1st Frame
35
Powder Diffractometer
36
Simulated Diffraction Experiment
37
High Pressure Diffractometer
Detectors
  • Instrument design dominated by high pressure cell
  • Novel high pressure neutron scattering cell
    design based on the megabar piston cylinder cell,
    very stable along thrust axis
  • Unique cell design provides large detector
    coverage

Incident beam
Cell designed by Carnegie Institution of
Washington, Geophysical Laboratory.
Sample
38
High Pressure Diffractometer Parameters and
Performance
  • Atomic structure at pressures up to 100 Gpa
  • Moderator decoupled supercritical H2
  • Source-sample distance 15 m
  • Sample-detector distance 37 cm
  • Angular coverage 38-142?, 98-150? horizontal
  • 34? vertical
  • 5 times the highest pressure of current neutron
    diffractometers
  • 200 times the intensity of current high pressure
    neutron diffractometers

39
Time-of-Flight Inelastic Instruments
  • Two basic types direct geometry fixed Ei
    (e.g. HET chopper)
  • Indirect geometry fixed Ef (e.g. IRIS
    backscattering)

40
Q-w space accessible with proposed spectrometers
41
High Resolution Backscattering Spectrometer
  • Crystal analyzer (Si) with 84 m incident flight
    path
  • Achieves 2.2 meV resolution at the elastic
    position with
  • 250 meV bandwidth
  • Can operate up to 18 meV energy transfer with 10
    meV resolution
  • Unprecedented capabilities
  • Performance gains over comparable reactor
    backscattering instruments gt100 (depending on
    bandwidth needed)
  • High-Q option (with Si 311) 500x IN13 and 18x
    IRIS (with 3 times Q range and better resolution!)

2000-03452/arb
42
Fermi Chopper Spectrometers
2.5-m chopper spectrometer
6-m chopper spectrometer
43
10-100 meV Multi-Chopper Spectrometer
Detector locus
Sample
Guide
Counter-rotating dual-disk high-speed choppers
44
Multi-Chopper Spectrometer Parameters and
Performance
  • Atomic-scale dynamics in the 0-20 meV energy
    range
  • Moderator coupled supercritical H2
  • Source-sample distance 42 m
  • Sample-detector distance 5 m
  • Angular coverage ?30? horizontal
  • ?30? vertical
  • 1 bank extending to 150?
  • Ei (meV) ?E/Ei () flux-on-sample (n/cm2/s)
  • 30 3 1?106
  • 10 1?107
  • 2 3 7?105
  • 10 5?106
  • Factor of 100 more flux on sample than any other
    disk chopper
  • spectrometer at the same resolution and energy
    transfer
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