Introduction to SAXS at SSRL John A Pople Stanford Synchrotron Radiation Laboratory, Stanford Linear Accelerator Center, Stanford CA 94309 Everything You.

Slides:



Advertisements
Similar presentations
When to Utilize SAXS Small-Angle X-ray Scattering (SAXS)
Advertisements

SOMO Workshop, 20th Intl AUC Conference, San Antonio, TEXAS, 25th - 30th March, 2012 Small-Angle X-ray scattering P. Vachette (IBBMC, CNRS UMR 8619 & Université.
Bragg’s Law nl=2dsinΘ Just needs some satisfaction!! d Θ l
Lecture 11. Microscopy. Optical or light microscopy involves passing visible light transmitted through or reflected from the sample through a single or.
Lecture 20 X-Ray Diffraction (XRD)
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
Determination of Protein Structure. Methods for Determining Structures X-ray crystallography – uses an X-ray diffraction pattern and electron density.
IMAGE FORMATION  Introduction  The Invisible and Visible Image  Image Characteristics.
Spectroscopic Ellipsometry University of Texas at El Paso Lynn Santiago Dr. Elizabeth Gardner Chem 5369.
Crystallography and Diffraction Techniques Myoglobin.
Yat Li Department of Chemistry & Biochemistry University of California, Santa Cruz CHEM 146C_Experiment #3 Identification of Crystal Structures by Powder.
Lecture : 2 Light scattering and determination of the size of macromolecules.
Grazing incident X-ray Diffraction (XRD) X-rays are electromagnetic radiation with very short wavelength (  m), very suitable to do diffraction.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Properties of Multilayer Optics An Investigation of Methods of Polarization Analysis for the ICS Experiment at UCLA 8/4/04 Oliver Williams.
Tuesday, May 15 - Thursday, May 17, 2007
Formation of 2D crystalline surface phases on liquid Au-based metallic glass forming alloys S. Mechler, P. S. Pershan, S. E. Stoltz, S. Sellner Department.
Methods: Cryo-Electron Microscopy Biochemistry 4000 Dr. Ute Kothe.
Diagnostics for Benchmarking Experiments L. Van Woerkom The Ohio State University University of California, San Diego Center for Energy Research 3rd MEETING.
Introduction to PHOTON CORRELATION SPECTROSCOPY
Bridging the solution divide: comprehensive structural analyses of dynamic RNA, DNA, and protein assemblies by small-angle X-ray scattering By Rambo and.
Stanford - SSRL: J. Lüning W. Schlotter H. C. Siegmann Y. Acremann...students Berlin - BESSY: S. Eisebitt M. Lörgen O. Hellwig W. Eberhardt Probing Magnetization.
Beam Lines At SSRL Cathie Condron SSRL Scattering Workshop May 2007.
Neutron Scattering 102: SANS and NR
Time out—states and transitions Spectroscopy—transitions between energy states of a molecule excited by absorption or emission of a photon h =  E = E.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
Grazing Incidence X-ray Scattering from Patterned Nanoscale Dot Arrays D.S. Eastwood, D. Atkinson, B.K. Tanner and T.P.A. Hase Nanoscale Science and Technology.
X. Low energy electron diffraction (LEED)
Effective lens aperture Deff
Space Filling Geometry and Materials Science & Engineering Terry A. Ring University of Utah.
Unknown at first, these photons from innershell transitions have played a vital role in materials analysis.
Determination of grain sizes and porosity in nanophase vanadium oxide and V/Ce oxide with GISAXS and GIXR Aleksandra Turković Ruđer Bošković Institute.
Dynamics Neutron Scattering and Dan Neumann
The effect of poly(propylene glycol) on the formation of lyotropic liquid crystalline phases of amphiphiles containing glycerol head groups Shin-Hong Ou,
FEMTOSECOND LASER FABRICATION OF MICRO/NANO-STRUCTURES FOR CHEMICAL SENSING AND DETECTION Student: Yukun Han MAE Department Faculty Advisors: Dr. Hai-Lung.
PHYS 430/603 material Laszlo Takacs UMBC Department of Physics
Diffraction Basics Coherent scattering around atomic scattering centers occurs when x-rays interact with material In materials with a crystalline structure,
Lars Ehm National Synchrotron Light Source
Magnetization dynamics
Neutron Metrology for Fuel Cells David Jacobson, National Institute of Standards & Technology (NIST) Phenomena Probed in Hydrogenous Materials Very large.
FIG. 5.1 Multiple scattering is viewed as a random walk of the photon in diffusing wave spectroscopy (DWS)
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
Interaction of X-Rays with Materials
Page 1 X-ray crystallography: "molecular photography" Object Irradiate Scattering lens Combination Image Need wavelengths smaller than or on the order.
PC4250 Introduction to Surface Analysis Techniques.
Heterometallic Carbonyl Cluster Precursors Heterometallic molecular cluster precursor - mediate transport and growth of nanoscale bimetallic particles.
Page 1 Phys Baski Diffraction Techniques Topic #7: Diffraction Techniques Introductory Material –Wave-like nature of electrons, diffraction/interference.
Neutron Probes for the Hydrogen Economy David Jacobson, Terry Udovic, and Jack Rush, Muhammad Arif, National Institute of Standards & Technology (NIST)
Phase Contrast sensitive Imaging
LCLS Brian Stephenson, Materials Science Division, Argonne National Laboratory Steven Dierker, Department of Physics, University of Michigan Simon Mochrie,
Polymers (see Roe: Methods of X-ray and Neutron Scattering in Polymer Science (2000)) Polymers (see Roe: Methods of X-ray and Neutron Scattering in Polymer.
Low Angle X-ray Scattering (LAXS) for Tissue Characterization Dr M A Oghabian.
Microscopy Large Features ( »  ) Real Space: x Single Object
Peterson xBSM Optics, Beam Size Calibration1 xBSM Beam Size Calibration Dan Peterson CesrTA general meeting introduction to the optics.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Comparison b/w light and electron microscopes LIGHT MICROSCOPE ELECTRON MICROSCOPE Magnification can be done upto 2000 times Resolving power is less.
Presentation on.  There are many methods for measuring of fiber structure. Such as:  The absorption of infrared radiation  Raman scattering of light.
Energy-Filtered Transmission Electron Microscope (EFTEM)
Static Light Scattering Part 2: Solute characteristics
Polarization Dependence in X-ray Spectroscopy and Scattering
Acoustical Society of America Meeting
R. Hashimoto, N. Igarashi, R. Kumai, H. Takagi, S. Kishimoto
Biological nanocomposite materials
Light scattering method Introduction: The illumination of dust particles is an illustration of light scattering, not of reflection. Reflection is the deviation.
Complex Nanophotonics
Christopher B. Stanley, Tatiana Perevozchikova, Valerie Berthelier 
Coherent X-ray Imaging Instrument WBS 1.3
X-ray Correlation Spectroscopy Instrument
Jochen Zimmer, Declan A. Doyle, J. Günter Grossmann 
Presentation transcript:

Introduction to SAXS at SSRL John A Pople Stanford Synchrotron Radiation Laboratory, Stanford Linear Accelerator Center, Stanford CA Everything You Ever Wanted to Know About But Were Afraid to Ask SAXS

When should I use the Scattering Technique?

Ideal Studies for Scattering Global parameters, distributions; 1 st order Different sample states In-situ transitional studies Non destructive sample preparation Scattering good for: SolidMelted & Sheared Recrystallized

Ideal Studies for Microscopy Local detail Surface detail Faithfully represents local complexities Microscopy good for: E.g. if objective is to monitor the degree to which Mickey’s nose(s) and ears hold to a circular micromorphology… use microscopy not scattering

Forming a bi-continuous porous network with ligament width on the nanoscale by removing the less noble element from a binary alloy, in this case Ag-Au 200 nm 5 mins in conc HNO 3 60 mins Complementary Scattering and Microscopy

Scattering: Neutrons or Photons? X-rays Neutrons Neutron scattering: Deuteration allows species selection X-ray scattering: Relatively small sample quantities required Relatively fast data acquisition times - allows time resolved effects to be characterized Sensitive to nuclear scattering length contrast Sensitive to electron density contrast

Scattering: Neutrons or Photons? Neutrons: Deuteration allows species selection AtomScattering lengthIncoherent scattering (x cm 2 ) (x cm 2 ) 1 H D This essentially permits a dramatic alteration to the ‘visibility’ of the tagged elements in terms of their contribution to the reciprocal space scattering pattern

Scattering: Neutrons or Photons? = 0% = 300% SANS patterns Photos of deformation

X-rays:Order of magnitude better spatial resolution Fast data acquisition times for time resolved data Scattering: Neutrons or Photons? Oscillatory Shearing of lyotropic HPC – a liquid crystal polymer

X-ray Scattering: Transmission or Reflection? Transmission geometry appropriate for: Extracting bulk parameters, especially in deformation Weakly scattering samples: can vary path length Need to be conscious of: Constituent elements, i.e. absorption cutoffs Multiple scattering Area of interest: surface effect or bulk effect

X-ray Scattering: Transmission or Reflection? Reflection geometry appropriate for: Films on a substrate (whether opaque or not) Probing surface interactions

X-ray Scattering: SAXS or WAXS? No fundamental difference in physics: a consequence of chemistry WAXS patterns contain data concerning correlations on an intra- molecular, inter-atomic level (0.1-1 nm) SAXS patterns contain data concerning correlations on an inter-molecular level: necessarily samples where there is macromolecular or aggregate order (1-100 nm) As synthesis design/control improves, SAXS becomes more relevant than ever before

X-ray Scattering: SAXS or WAXS? Experimental consequences WAXS: Detector close to sample, consider: Distortion of reciprocal space mapping Thermal effects when heating sample No ion chamber for absorption SAXS: Detector far from sample, consider: Absorption from intermediate space Interception of appropriate q range

What can I Learn from a SAXS Pattern?

Recognizing Reciprocal Space Patterns: Indexing Face centered cubic pattern from diblock copolymer gel

Face centered cubic Recognizing Reciprocal Space Patterns: Indexing Real space packing Reciprocal space image (unoriented domains) Body centered cubic Hexagonal Normalized peak positions ≡1; =√2; =√3 ≡1; =√4/3; =√8/3 ≡1; =√3; =√4

Recognizing Reciprocal Space Patterns: Preferential Orientation Real space packing Reciprocal space image Randomly aligned rods Preferentially aligned rods Hydrated DNA

Extracting Physical Parameters from X-ray data q  I(q) I(  )  q

Extracting Physical Parameters from X-ray data Molecular size: Radius of gyration (R g ) Guinier plot R g 2  ln I(q) / q 2 I(q) = I(0) exp [-q 2 R g 2 / 3] Guinier region: q < 1 / R g ln I(q) q2q2

Extracting Physical Parameters from X-ray data Molecular conformation: Scaling exponent Guinier plateau Intermediate region ln I(q) ln q Rod Sphere Coil in good solvent q -1 q -5/3 q -4 Gradient of profile in intermediate region implies fractal dimension of scattering unit

Molecular Conformation in Dentin q  SAXS pattern pulpDEJ John H Kinney Department of Preventive and Restorative Dental Sciences, University of California, San Francisco, CA 94143

Molecular Conformation in Dentin

Shape change of mineral crystallites from needle-like to plate-like from pulp to dentin-enamel junction (DEJ). pulpDEJ needle-like plate-like Dentinogenesis imperfecta (DI) teeth shown to exhibit impaired development of intrafibrillar mineral: characteristic scattering peaks are absent from the diseased tooth. Molecular Conformation in Dentin

Extracting Physical Parameters from X-ray data Kratky plot Molecular conformation: Persistence length of coiled chain I(q) q 2 q q* persistence length = 6 / (  q*)

q  Extracting Physical Parameters from X-ray data I(  )  Azimuthal profile Molecular orientation: Orientation parameter P 2 =  I(s,  ) P 2n (cos  ) sin  d   I(s,  ) sin  d  Normalized: -0.5 < P 2 < 1

Orientation parameters: 0 < P 2 < 0.3 Axis of orientation Measuring the degree and inclination of preferential molecular orientation in a piece of injection molded plastic (e.g. hip replacement joints). ~ 1500 WAXS patterns Molecular Orientation in Injection Moldings Marks the injection point

SSRL Beamline 1-4: SAXS Materials Science shutter beam defining slits ion chambers sample stage guard slits CCD detector optical rail & table N 2 supply X-rays

linear eicosanol (C 20 H 42 O, MW = 298) Study phase transitions of Langmuir monolayers of mixed fatty alcohols in terms of molecular branching and surface tension branched eicosanol (C 20 H 42 O, MW = 298) increasing surface pressure: 0 to 40 mN/m q (/nm) Linear Eicosanol Langmuir trough Gold mirror x-ray path Surface tension sensor Rheology of Straight and Branched Fatty Alcohols