LoKI – A SANS Instrument for Materials Science and Soft Matter LoKI Kickoff Meeting, ESS Andrew Jackson www.europeanspallationsource.se January 29, 2014.

Slides:



Advertisements
Similar presentations
Unit 6 Fuel Cells
Advertisements

Evgeny Karpushkin, Andrey Bogomolov WSC-9, Tomsk, Feb 2014
FLAME SPECTROSCOPY The concentration of an element in a solution is determined by measuring the absorption, emission or fluorescence of electromagnetic.
Nature provides us of many examples of self- assembled materials, from soft and flexible cell- membranes to hard sea shells. Such materials.
ESS and Reflectometry SAC Report 22 nd May The Reflectometry STAP John Ankner (SNS) Richard Campbell (ILL) Bob Cubitt (ILL) Robert Dalgliesh (ISIS)
Utilizing Carbon Nanotubes to Improve Efficiency of Organic Solar Cells ENMA 490 Spring 2006.
COMPUTATIONAL MODELLING AND EXPERIMENTAL ANALYSIS OF FLOWS IN PEM FUEL CELLS Robert A. Blewitt and Dr John S. Shrimpton Thermofluids Section, Department.
A Microfluidic System for Controlling Reaction Networks In Time Presented By Wenjia Pan.
Bologna on 28 May 2008 – IP EUROTRANS WP1.51 IE - Institute for Energy Petten - The Netherlands
Solid Target Options NuFACT’00 S. Childress Solid Target Options The choice of a primary beam target for the neutrino factory, with beam power of
Mechanical and fluidic integration of scintillating microfluidic channels into detector system 1 Davy Brouzet 10 th September 2014.
HEAT TRANSFER CHALLENGES IN PROCESS INTENSIFICATION
Neutron Scattering 102: SANS and NR
Science and Technology of Nano Materials
ISIS Second Target Station
ANSTO is Australia’s only nuclear science and technology facility
Abstract A time resolved radial profile neutron diagnostic is being designed for the National Spherical Torus Experiment (NSTX). The design goal is to.
Small Angle Neutron Scattering SANS (Neutron scattering) by Samuel Ghebru.
Solar observation modes: Commissioning and operational C. Vocks and G. Mann 1. Spectrometer and imaging modes 2. Commissioning proposals 3. Operational.
Benjamin Welle Stanford University Grant Soremekun Phoenix Integration
Dynamics Neutron Scattering and Dan Neumann
Infrared Spectroscopy using Quantum Cascade Lasers Peng Wang and Tom Tague Bruker Optics, Billerica, MA Laurent Diehl, Christian Pflügl and Federico.
Selective Laser Sintering of Graphite Composite Bipolar Plates for PEM Fuel Cells Nannan Guo, Ming C. Leu Center for Aerospace Manufacturing Technologies,
Potential Portuguese Contributions to the ESS Project Areas and topics of interest for the ITN Pedro Vaz (ITN) Workshop “Towards a Portuguese Participation.
Neutron detection in LHe ( HMI run 2004) R.Golub, E. Korobkina, J. Zou M. Hayden, G. Archibold J. Boissevain, W.S.Wilburn C. Gould.
Mohraz Lab Colloid Science and Complex Fluids Engineering Mohraz Lab Colloid.
Structure Update Installation & Building Update Revisions Outlined Costs Revisited (since given to Gina) Jeff Nelson Fermilab.
This basic spectrophotometer training session should enable you to know: Basics of how a Spec’ Works What the Individual Components Actually Do Commonly.
ESS - SANS Instrumentation pulsed source SANS, using a wide range of wavelengths, uses more of the available flux than a continuous source. For same time.
Past and Future Insights from Neutron Scattering Collin Broholm * Johns Hopkins University and NIST Center for Neutron Research  Virtues and Limitations.
Neutron Scattering Group February, 2001 A High Performance Instrument for the Single Crystal Spectroscopy at the Pulsed SNS. n What is the spectrometer.
TC Straw man for ATLAS ID for SLHC This layout is a result of the discussions in the GENOA ID upgrade workshop. Aim is to evolve this to include list of.
Mitglied der Helmholtz-Gemeinschaft Jörg Wolters, Michael Butzek Focused Cross Flow LBE Target for ESS 4th HPTW, Malmö, 3 May 2011.
CLIC Stabilisation Day’08 18 th March 2008 Thomas Zickler AT/MCS/MNC/tz 1 CLIC Quadrupoles Th. Zickler CERN.
Acquisition of major research instrumentation for advanced photoelectron spectroscopy with spin, angle and spatial resolution Acquisition of major research.
BENE/EURISOL-DS Joint Meeting, CERN, SwitzerlandFebruary 22, Progress in the Liquid Mercury Multi-MW Target Design Studies Y. Kadi On behalf of.
HYSPEC IDT Polarized Beam Mode for the Hybrid Spectrometer (HYSPEC) at the Spallation Neutron Source. Outline Polarization analysis and the HYSPEC place.
ESS TDR Internal Review Chapter and 12. October 2012 Oliver Kirstein.
Werner Schweika, Nicolo Violini, Earl Babcock Michael Meissner Andreas Houben, Philipp Jacobs Gunnar Svennson, Xiaodong Zou, Niklas Hedin, Mats Johnsson,
Phase 1 Design for LOKI at ESS: performance evaluation of suitable detector technologies Or how to build detectors for ESS Kalliopi Kanaki Andrew Jackson.
SCIENCE FAIR CATEGORIES MIDDLE SCHOOL :
October, 2001 Hybrid Spectrometer for Single Crystal Studies at the Pulsed SNS: an update. n Principal features of the proposed hybrid spectrometer. n.
Neutron ESS. Status Status #2 Conclusion: Estia is through and FREIA is difficult to kick out. In principle a third reflectometer.
Target Systems and Monolith Design Update Rikard Linander Group Leader Monolith and Handling April 2, 2014.
DECam Spectrophotometric Calibration DECam calibration workshop, TAMU April 20 th, 2009 Jean-Philippe Rheault, Texas A&M University.
The ESS Target Station Eric Pitcher Head of Target Division February 19, 2016.
The ESS Target Station F. Mezei ESS target division NPPatLPS, 2013.
Material Downselect Rationale and Directions Gregory Harry LIGO/MIT Kavli Institute for Astrophysics and Space Technology On behalf of downselect working.
Development of Electrolysis System Powered by Solar-Cell Array to Supply Hydrogen Gas for Fuel-Cell Energy Resource Systems Priambodo, P; Yusivar, F; Subiantoro,
UV/VIS SPECTROSCOPY.
ESS Gold A Proposal for a Next Generation European Neutron Source
Science Fair Categories
Droplet Dynamics of a Flowing Emulsion System in a Narrow Channel
A cold neutron beam facility for particle physics at the ESS
Kinetic Theory.
LCLS Instrument Development
Utilizing Carbon Nanotubes to Improve Efficiency of Organic Solar Cells ENMA 490 Spring 2006.
The NPDGamma Experiment at the SNS FnPB
Controlling Sensors Efficiently with MCUs
Solid-liquid and flow cells
ESS Freia Scope Setting ESS - Lund - 17/10/2016.
MIRACLES budget: Summary of the 3 configurations
(Beam) Commissioning Plan
Path to BEER upgrades STAP meeting – Phase 2.
Mageleka MagnoMeter™ XRS
Scope Setting Meeting MIRACLES
Test Beamline System Requirements and Charge to PDR Committee
Computed Tomography (C.T)
C.6 Liquid Crystals The liquid crystal state Liquid Crystal Examples
LoKI Science Case and SEE Priorities
Presentation transcript:

LoKI – A SANS Instrument for Materials Science and Soft Matter LoKI Kickoff Meeting, ESS Andrew Jackson January 29, 2014

What is “Materials Science”? GEO SCIENCE LIGHTING FUNCTIONAL FABRIC FUNCTIONAL FABRIC MEDICINE SOLAR ENERGY SOLAR ENERGY BIO FUEL TRANSPORT COSMETICS FUNCTIONAL FOOD FUNCTIONAL FOOD MOBILE PHONES PACE- MAKERS IMPLANTS NEW MATERIALS NEW MATERIALS Materials Science Shapes Our Daily Lives CONSTRUCTION MATERIALS CONSTRUCTION MATERIALS

Wikipedia says... Soft matter is a subfield of condensed matter comprising a variety of physical states that are easily deformed by thermal stresses or thermal fluctuations. They include liquids, colloids, polymers, foams, gels, granular materials, and a number of biological materials. What is Soft Matter? 3 page

Fluid Flow The flow of complex fluids through complex geometries is relevant to many industrical processes including polymer processing and oil recovery. Microfluidic devices are increasingly used for chemical and pharmaceutical discovery, production and processing. There is a need to understand structural effects of flow both for practical puroposes and to compare with fluid flow models. Measuring the deformation of polymer chains allowing development of new models of polymer flow (Clarke et al. (2010) Macromolecules 43, 1539) Fluid thread breakup under microfluidic confinement (Cabral group, Imperial College) Shear Banding in CTAB wormlike micelles providing confirmation of rheological model. (Helgeson et al. (2009) J. Rheol 53, 727)

Multiple Length Scales & Kinetics Double network hydrogels provide strength and resiliance together with high water content. Gel structure forms over multiple length scales. Kinetics of gelation can be rapid needing sub-second time resolution. Neutrons provide the structure of each component in the presence of the other. Swelling of a double network hydrogel designed for use as a cornea replacement. (Frank Group, Stanford) Amyloid fibrils have been associated with more than 20 human diseases including Alzheimer’s and Parkinson’s diseases and rheumatoid arthritis. Fibril formation and growth is a multi-length scale problem and to understand methods of formation and inhibition the structural evolution must be observed.

In-Operando Behaviour Lithium Ion Batteries are a crucial technology for the expansion of electric vehicle use and for mobile computing. Higher energy densities could be achieved with alternative anode materials and new electrolytes. Analysis of operating devices allows the monitoring of nano- and micro-structural change. Dendrite growth in lithium metal anode batteries observed by x-ray microtomography. (Harry et al. (2013) Nature Materials 13, 69) Organic Solar Cells promise to provide cheap and accessible solar energy. The lifespan and efficiency of the devices depends on the nano-structure of the bulk heterojunction polymer mixture. Understanding the structural evolution under operation guides development of new devices.

The Source 17 Countries Brightest neutron source 5MW 2.86 ms 14 Hz First neutrons instruments by B€

8 Goals A broad Q range, high flux SANS instrument for materials science and soft matter Science Based Goals Rapid data collection / short counting times to enable kinetics Probe broad size range to examine hierarchical structures Small sample volumes for scanning, biological and complex samples Integrated flexible sample environment for non-equilibrium studies Integration of complementary techniques experimentally and in data analysis Simplicity of operation to allow users to focus on science

9 Goals Technological Goals Broad simultaneous Q range with Q max /Q min = 1000 Good Q resolution over the whole Q range High flux making best use of ESS source Single pulse scattering measurements Optimized use of new detector technologies A broad Q range, high flux SANS instrument for materials science and soft matter

10 Goals Design Constraints Avoid line-of-sight (background) Bandwidth vs Time Resolution (Q resolution) Space (sample environment) A broad Q range, high flux SANS instrument for materials, soft matter and bio-science. Wavelength-Distance Space used by LoKI Conclusion Detectors between 20 m and 30 m

11 Goals A broad Q range, high flux SANS instrument for materials science and soft matter Wavelength-Distance Space used by LoKI Require good Q resolution across whole Q range - high angle to reach high Q with long wavelengths. Need broad Q range - large solid angle of detectors and broad wavelength band. High spatial resolution at low angles to reach low Q

12 Overview Bender: r = 78 m l = 4 m 4 channels m = 3 Guide: 3 cm x 3 cm m=1 Collimation: Up to 10 m A 1 = 20 mm, 10 mm, 8 mm, 4 mm Variable Opening Choppers SDD: 2m, 5m, 10m SDD: ~ m Optional Focussing Optics

13 Bender Performance 78 m radius 4 m length 3 cm x 3 cm 4 channels m = 4 Bender Guide CollimationChopper 1Chopper 2 Avoid line of sight before start of collimation

14 Wavelength Selection Variable opening double disc choppers at 6.5 m and 9.8 m 14 Hz Å 7 Hz Å

15 Sample Position A flexible space with 2.5 m along the beam and 3 m perpendicular to the beam A system of sample environment pallets that can be quickly interchanged allowing offline setup of equipment Space for magnets, rheometers and shear cells, pressure cells, sample changers, auto-sampling robots, flow-through cells... whatever the user can think of! Space for complementary measurement techniques

16 “ Lined Tube ” Detectors Q range of 1m diameter high angle detector 0.03 Å -1 < 1.0 Å -1 using 3Å Å neutrons 12 Å 2 Å

17 “ Window Frame ” Detectors Front: 3 m x 3 m with 1 m x 1m hole Middle: 2.4 m x 2.4 m with 0.5 m x 0.5 m hole Back: 0.5 m x 0.5 m Accessible Q ranges with 3 Å Å neutrons

18 Performance Scattering from 1mm H 2 O using “ Window Frame ” detector layout

19 Risk Management Risk : Detectors will not be available. Mitigation : This is a common risk for all ESS instruments that require large areas of detector given the lack of 3He options (availability, count rate). As such it is a high priority for ESS to develop such systems and current progress is good. In the case of LoKI, the initial design phase will progress with multiple possible detector layouts and the final technology choices can be made months after the start of the construction project. This should provide sufficient opportunity for detector developments to be advanced to a stage where that decision is possible. Risk : Shielding will not be sufficient to provide a low enough instrumental background Mitigation : This is again a common risk for all the short (< 60 m) instruments at ESS and the optics group is already working to address it. During the engineering design phase we will work closely with the optics group to determine exact requirements and design the shielding solution.

20 Costing 3He Detectors in Window Frame layout 20 M€ 10B Detectors in Window Frame layout 14.5 M€ 10B Detectors in Lined Tube layout 12 M€ Notes: Costing for 10B detectors assumes production pricing i.e. R&D costs are borne by detector group Costs are higher than in proposal based on increase in chopper cost as advised during review

21 Summary LoKI will provide A world leading SANS instrument for the ESS with high flux, wide simultaneous Q range, a flexible sample area and opportunity for enhancement with focussing optics. Beam sizes as small as 2mm will be routinely accessible allowing small sample volumes and scanning experiments. The ability to perform “ single-shot ” kinetic measurements on sub- second time scales The ability to perform stroboscopic measurements with a time resolution of the pulse length.