SAXSSAXSSmall Angle X-ray Small Angle X-ray ScatteringScattering

Talia Zemach (2002)Talia Zemach (2002)

Raanan Kalifa (2003)Raanan Kalifa (2003)

Rami Shnaiderman (2005)Rami Shnaiderman (2005)

Materials Engineering, BGUMaterials Engineering, BGU

Lecturer: Prof. Jacob ZabickyLecturer: Prof. Jacob Zabicky

Introduction—the scale of thingsIntroduction—the scale of thingsScattering from

1. X-rays

2. Neutrons

3. Electrons

4. Light

is used in many disciplines to study a vast range of materials.

Electromagnetic radiation can be used to obtain information about materials of dimensions of the same order as the wavelength of the radiation passing though the material. For example, an ordinary glass of milk vividly illustrates this principle. In normal visible light the milk appears as a continuous, ‘milky’ white fluid. However, place the same glass of milk in ultraviolet “black” light and it appears as an emulsion of particles because the wavelength of the UV light is similar to the dimensions of the butterfat that is dispersed as tiny drops in the serum.

Introduction—light scatterimgIntroduction—light scatterimg

Around the turn of the 20th century, Röntgen discovered radiation with wavelength much shorter than that of visible light (less than 1 nm) – the X-rays. Soon after that von Laue and his associates discovered that crystals scatter X-rays in distinct patterns (diffraction).

It was soon recognized that these patterns give direct insight into the structure of the materials that caused the scattering, allowing us to determine the morphology and size of the particles (e.g.,

molecules) assembling the mater .

Scattering experiments usually consist of irradiating a sample with highly coherent X-ray radiation and measuring the resulting scattering pattern.

Introduction—X-rays scatterimgIntroduction—X-rays scatterimg

The reciprocity law The reciprocity law

The reciprocity lawThe reciprocity law: :

The larger the diffraction angle the smaller the length The larger the diffraction angle the smaller the length scale probed and viceversa.scale probed and viceversa.

Wide angle X-ray scattering (WAXS) is used to determine crystal structure on the atomic length scale while small-angle X-ray scattering (SAXS) or small-angle neutron scattering (SANS) are used to explore microstructure on the colloidal length scale .

The larger the diffraction angle the smaller the length The larger the diffraction angle the smaller the length scale probed and vice versa.scale probed and vice versa.

The difference between small angle scattering (SAXS) and wide angle scattering (WAXS) is in the scale of the sample and consequently

the size of the angle .

–wavelength of X-rayd – distance between

relevant parts of the analyzed sample

–half the angle between the diffracted and transmitted beams

The reciprocity law The reciprocity law

For example,

d = 250 Åλ = 1.5 Å (fixed)

corresponds to

= 0.17° = = 0.030 rad

What is SAXS?Small angle X-ray scattering (SAXS) is a well-established chatacterization tool that has been around for about 70 years. It is "special" in terms of the distinction between SAXS and regular wide-angle X-ray scattering by virtue of the location of the scattering of interest. This is typically at small angles in the vicinity of the primary beam and extending to less than 2 degrees for standard wavelengths. The scattering features at these angles correspond to structures ranging in size from tens to thousands of angstroms.

Closer inspection shows that the X-ray is diffracted due to regularly spaced scattering objects, e.g. atoms in a solid matter, that cause differences in electron density. For diffraction to occur the spacing between the objects must be equal to an integral multiple of the wavelength of the probing radiation, making the X-rays perfect for investigation of nano-structures.

Why not light scattering?Frequently we need to look at bulk materials which are opaque to

visible light.The wavelength of light is much larger than that of X-rays (or

neutrons), which makes light scattering adequate for much larger structures (like phases in blends of elastomers).

Why not electron microscopy ?The need to produce very thin slices for electron microscopy can

destroy the very thing we want to observe.

Why SAXS?While SANS is usually a possibility, it certainly is less straightforward

than SAXS.There are cases where SAXS is either the best or the only source of

information that is needed on some materials.

SAXS experiments• The electrons in the sample scatter off X-rays.• Being X-rays of high energy small scattering angles are

possible.• A long instrumental setup is needed to measure the small

angles.• Scattered and transmitted X-rays are detected on an area

detector, for example, a charge-coupled device (CCD), and the display is sent to a computer for processing.

• The scattering angle is determined from the distance of the pixel to the center of the display.

• The scatering angle allows estimation of the radius of giration (Rg) and the particle shape.

• The result of a SAXS experiment is essentially the intensity of the Fourier transform of the electron density and must be interpreted in order to determine morphology, size, structure, physical properties (volume, area, weight ).

• DirectDirect methods methods yield information based on interpretation of the clean (background corrected) data with no further manipulation. However, all these parameters are based on well-defined assumptions such as uniform density within the so-called particle, uniform density in the background, sharp interfaces between the two, etc.

• When these assumptions do not apply one can carry out a Fourier transform of the data to get real space information. However, not as in electron microscopy, a fundamental problem with any scattering experiment is that two different morphologies can, in theory, give identical scattering patterns. Generally, one cannot reconstruct the exact microstructure uniquely from a SAXS pattern because in a scattering experiment only the scattered radiation intensity can be measured and all phase information is lost .

• The scattering intensity is proportional to the number of scattering elements in the irradiated volume Np(1/q). Then,in small angle scattering we can consider a generalized rule that describes the behavior of scattered intensity as a function of Bragg’s size “d” or ‘r” that is observed at a given scattering angle 2θ , where r =1/q.

•When these assumptions do not apply one can carry out a Fourier transform of the data to get real space information (such as obtainable by electron microscopy).

A scattering experiment

The detected patterns may be isotropic, oriented, bimodal, etc.

SAXS CCD and processed results

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

SAXS processed results

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

It is helpful to recognize some of the more typical SAXS patterns of isotropic systems, i.e. whether macroscopic orientation exists or not in the scattering volume.

SAXS result on the CCD and in q space

A bright ring means there is a periodic structure in that object with the corresponding repeat spacing .

Intense scattering over a range of angles means the structure is ordered on that length scale but not periodic.

SAXS Data Analysis-Direct methods.◊ Guinier region: ◊ At very small angles, the shape

of the scattering can be used to give us an idea of the radius of gyration of any distinct structures that are on this range of length scale.

◊ At higher angles, if we had a system of relatively uniform particles, dilute enough for mutual interactions, we might be able to see broad peaks that would also give us information on the shape of the particles.

q = 2πsin/Dmin = 2π/qmin

SAXS Data Analysis.◊ Porod region:

At higher angles, the shape of the curve gives information on the surface-to-volume ratio of the scattering objects. This can also be used to obtain information on the dimensions of the scattering particles.

◊ INVARIANT : The area under the curve is a measure of the amount of scattering material seen by the X-ray beam. Changes in the invariant are useful to follow crystallization in polymeric materials.

q = 2πsinθ/λD max = 2π/qmax

Do = 2π/qo

Examples of data analysis-direct methods

1E-3 0.01 0.11E-3

0.01

0.1

1

10

100

1000

I(q

)/

²

q (Å -1)

R=10 r

r

R, Df =2

I q-Df

L. Barre, IFP France

Examples of data analysis-direct methods

1E-3 0.01 0.11E-3

0.01

0.1

1

10

100

1000

I(q

)/

²

q (Å -1)

R=10 r

r

R, Df =2

I q-Df

L. Barre, IFP France

Schematics of an X-ray scattering Schematics of an X-ray scattering assemblyassembly

And in more detail…

Instrumentation

Instrumentation

Applications

Many applications of the SAXS technique are found in :

* Structural biology (proteins, muscles, lipid vesicles).* Polymer science.* Colloidal chemistry.* Materials science (crystalline alloys, amorphous materials,

single crystals, porous materials, liquid crystals).* Chemical analysis.

*For monodisperse particle systems*Radius of gyration of particle, of rod or platelet, i.e. size parameter

*Particle shape in solution ﾐ comparison of modelled vs. experimental scattering curve

*Radial electron density distribution, e.g. of micelles *Molecular weight of particle, of unit length (rods), or unit area (plates)

*For concentrated solutions*Solution structure function

*For polymers*in solution: persistence length, degree of coiling

*in bulk: domain structure (crystalline vs. amorphous), lattice structure*For liquid crystals ﾐ low-dimensional systems

*Lattice symmetry and dimensions *Degree and nature of long-range disorder

*For powders *Specific inner surface / surface-to volume ratio of inhomogeneities

Applications

Applications

A SAXS pattern of a surfactant templated mesoporous silicate

Applications

Latex particles of uniform size in solution can be described as a dense core surrounded by a hairy halo of loose tails.

Applications

In the presence of Ca(II), gelsolin undergoes a structural change that allows recognition and binding to actin.

SAXS Data on Gelsolin Ca2+

Å

140

120

100

80

60

40

20

0

Rel

ativ

e In

ten

sity

0.250.200.150.100.05 Q (

-1)

Ca2+_Gelsolin EGTA_Gelsolin

Applications

QuickTime™ and aTIFF (LZW) decompressor

are needed to see this picture.

Diffraction pattern of a highly aligned lipid (DMPC) in the Pb ｫ phase at constant grazing angle at 20 °C. Letter A shows the in-plane reflections due to the ripple structure (distance lambda), letter B gives the off-plane reflections due to the lamellar repeat distance d (see lower insert). C denotes the specular reflectivity peak. QuickTime™ and a

TIFF (LZW) decompressorare needed to see this picture.

To Sum it upTo Sum it up……

• SAXS allows studying nano-structured materials (1-100nm). on their typical length scale.

• The problem of small-angle analysis consists of deducing the structural features, such as size, shape or mass, from the interference pattern.

To Sum it up - Main To Sum it up - Main advantages. advantages. Good statistics: the volume of the material which is

sampled is in the range from 105 to 107µm3, depending on the material, wavelength of the X-rays and focusing of the beam. Thus a very large number of particles are averaged in the measured data.Quantitative measurements: from a SAXS spectrum, an average size of the particles can be obtained in a straightforward and automated manner. The volume fraction of the objects can be obtained too, provided that their composition is well known.In-situ measurements: the sample size and the measuring times enable easy real time studies during heating or deformation, and detailed information can be obtained on precipitation kinetics or phase changes during straining.Nondestructive for polymers.

A recent developmentA recent developmentThe use of synchrotron radiationsynchrotron radiation sources in SAXS studies increases the resolution of the experiments and decreases the acquisition times, leading the way for new types of experiments, notably those involving fast in situ measurements (with events of the order of a few seconds), in temperature or deformation, yielding time-resolved measurements as well as space-resolved studies of heterogeneous samples.

ReferencesReferences•http://physics.queensu.ca/~marsha/SAXS.html

•http://coecs.ou.edu/Brian.P.Grady/saxs.html•http://www-ssrl.slac.stanford.edu/~saxs/

•http://www.molmet.com•http://www.jjxray.dk/sxupg.html

•http://www.hecus.at/image/i_c_10_02.gif•http://scattering.tripod.com/

•Encyclopedia of Materials, Microscopic, spectroscopic and physical techniques

•Michette/Buckly, X-Ray Science and Technology, 1993.

•A small angle X-ray Apparatus for studying biological macromolecules solution, J. Appl. Cryst., (1998) 31, 533-543.

•Kirk-Othmer’s Encyclopedia of Industrial Chemistry, Structure analysis by diffraction.