The Importance of Refractive Index When using Laser Diffraction

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The Importance of Refractive Index When using Laser Diffraction Mark Bumiller mark.bumiller@horiba.com

Fraunhofer Approximation

Mie Theory RI 1.60 0.0i, in water, RI 1.33

Mie vs. Fraunhofer 1.E+05 1.E+04 100 μm Relative Intensity 1.E+03 1.E+02 1.E+01 1.E+00 1.E-01 1.E-02 1.E-03 3 μm 3.0 µm by Mie 3.0 µm by Fraunhofer 100.0 µm by Mie 100.0 µm by Fraunhofer 1.E-04 0.01 0.1 1 10 100 Angle in degrees Figure A.3 -- Comparison of scattering patterns of non-absorbing particles according to Fraunhofer and Mie calculations (N p = 1,59 0,0; n water = 1,33; wavelength = 633 nm)

Practical Application of Theory: Mie vs. Fraunhofer for Glass Beads

Practical Application of Theory: Mie vs. Fraunhofer for CMP Slurry

Influence of Particle Size on Angular Light Intensity Scattering Patterns

Influence of Imaginary Parts of RI (Absorbancies)

Refractive Index Refractive Index is defined by two components Real and Imaginary RI = n + ik Where: N = real component, velocity of light in a vacuum/ velocity of light in the particle = c/v p c = speed of light in vacuum Vp = speed of light in particle (liquid, air) k = the extinction coefficient of the material i = -1

RI: Real Component Real component from published tables or measured using Snell s Law n sin = n sin where: n= RI of air = angle of incidence n = RI of particle = angle of refraction n Light Path n n sin = n sin

n is Frequency Dependent 1.53 1.51 Remember the LA-950 has two light sources Red = 650 nm Blue = 405 nm In this example 1.53 vs. 1.51 Not very important Could matter for sub-micron pigments Sellmeier equation

RI: Imaginary Component Imaginary component (k) in Mie equation is the extinction coefficient of the particle. Reduction of transmission of optical radiation caused by absorption and scattering of light. k = Where: k = the extinction coefficient = the absorption coefficient = the wavelength of light used Light Path Particle Absorption coefficient ( ) = reciprocal distance light penetrates surface & be attenuated to 1/e of original intensity, about 37%. Opaque particles have high coefficient.

RI: Imaginary Component 100% Intensity 1 / e = 37% d Distance into medium 1 / d = k = ( Example: for a value of k = 0.1 k = [ ] = 0.05 x [1 / d] = 0.1 = k d = 0.05 / 0.1 = 0.5 micron

RI: Imaginary Component For transparent particles use 0 for the imaginary component For slightly opaque materials use 0.01 or 0.1 For opaque materials use 1.0 or higher Values can exceed 1.0 (see below*) *http://www.ee.byu.edu/photonics/opticalconstants.phtml

Refractive Index Effect Most pronounced when: Particles are spherical Particles are transparent RI of particle is close to RI of fluid Particle size is close to wavelength of light source Least pronounced when: Particles are not spherical Particles are opaque RI of particle is larger than RI of the fluid Particle size is much larger than wavelength of the light source

Older HORIBA Software: RI Kernels If n = 1.33 (water) and n = 1.60 (particle) Relative refractive index (RRI) : 1.60/1.33 = 1.203 Transparent particles: k = 0 Kernel function:120-000rri n n Suspending medium Particles somewhat opaque: then k > 0 KERNEL function: 120-020rri If powder, relative index: n = 1.0 (air) and n = 1.60 (particle), RRI: 1.60/1.0 = 1.60 Kernel function: 160-000rri or 160-020rri particle

Practical Approach Measure sample once Change RI Does result change significantly? No: stop worrying Yes: keep working For LA-950 users: determine real component, vary imaginary component to minimize residual R value. Oops, gave the plot away

Dissolve sample at different concentrations Plot conc. vs. RI Extrapolate to infinite concentration Abbe Refractometer 1.8 Refractive Index 1.6 1.5 1.4 1.3 0 0.2 0.4 0.6 0.8 1.0 Concentration

Becke Lines Bright line is called the Becke line and will always occur closest to the substance with a higher refractive index

Becke Line Test As you move away from the thin section (raising the objective or lowering the stage), the Becke Line appears to move into the material with greater refractive index. A particle that has greater refractive index than its surroundings will refract light inward like a crude lens. A particle that has lower refractive index than its surroundings will refract light outward like a crude diverging lens.

Becke Line Test

Luxpop.com Note RI is dependent on wavelength of light. Can adjust RI for red & blue light, but only need to for small, absorbing particles.

RI of Polymers http://www.texloc.com/closet/cl_refractiveindex.html

Google Search

Mixtures Larsen, E.S., Berman, H., The Microscopic Determination of the Non-Opaque Minerals, Second Edition, United States Department of the Interior, Geological Survey Bulletin 848, 1934, US Government Printing Office, Washington, DC.

Mixtures

Anisotropy Also called birefringence Many crystals have different RI as inspected through different planes. Use average, consider flow alignment I would rather eat French food

Uniaxial vs. Biaxial Materials Biaxial birefringence, also known as trirefringence, describes an anisotropic material that has more than one axis of anisotropy where n o and n e are the refractive indices for polarizations perpendicular (ordinary) and parallel (extraordinary) to the axis of anisotropy respectively. 3 Elert, Glenn. "Refraction". The Physics Hypertextbook. http://hypertextbook.com/physics/waves/refraction/.

Scary Example: Is the Small Peak Real? Starch sample Low imaginary

Scary Example: Is the Small Peak Real? Starch sample High imaginary

Scary Example: Is the Small Peak Real? Starch sample Zero imaginary The old secondary scattering trick?

Effect of RI: Cement Fixed absorbance, vary real Fixed real, vary absorbance

Chi Square and R Parameter yi The measured scattered light at each channel (i) of the detector. y (xi) The calculated scattered light at each channel (i) of the detector based on the chosen refractive index kernel and reported particle size distribution. σi The standard deviation of the scattered light intensity at each channel (i) of the detector. A larger σi indicates lower reliability of the signal on a given detector. N The number of detectors used for the calculation

Using R Value for i

Changing RI

Changing RI

Changing RI

Using R Value for i

Using R Value for i Real component = 1.57 via Becke line Vary imaginary component, minimize Chi square & R parameter

Automation by Method Expert Analytical conditions Calculation conditions View Method Expert webinar TE004 in Download Center

Automated RI Computation Real part study Need to fix imaginary part Set up to 5 real parts Software will compute all RI and display R parameter variation with RI selection

Automated RI Computation

Automated RI Computation

Automated RI Computation Imaginary part study Need to fix real part Set up to 5 imaginary parts Software will compute all RI and display R parameter variation with RI selection

Automated RI Computation Imaginary study

Summary Measure sample, recalculate w/different RI see how important it is Use one of the described approaches to determine the real component Recalculate using different imaginary component Choose result that minimizes R parameter, but also check if result makes sense You wish you had Method Expert by your side

Register to visit Download Center Application Notes Technical Notes Past webinars Bibliography And soon today s webinar mark.bumiller@horiba.com ian.treviranus@horiba.com It s All on the Website