Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. A graph of the structure factor at volume fractions fv=0.001, 0.2, and 0.5 as a.

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Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. A graph of the structure factor at volume fractions fv=0.001, 0.2, and 0.5 as a function of Dq=(kD)*2 sin(θ/2). The curve was calculated using the algorithm described by Tsang et al., 24 as the numerical Fourier transform of the Percus–Yevick pair correlation function (PCF). Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO

Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. Histogram of the size distribution of monodisperse silica beads (PSI 1.0) measured with transmission electron microscopy. Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO

Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. Simulated extended Huygens–Fresnel (EHF) model for optical coherence tomography (OCT) (green dashed line), experimental OCT curve (black solid line) fitted with a single exponential decay within the ROI for samples of 0.1 volume fraction: (a) 0.47-μm beads and (b) 1.60-μm beads. The simulated single scattering (Mie+PY) curve (blue dotted line) is plotted for reference. The exponential decay of the fits on the experimental curves is (a) μexp=5.0 mm−1 and (b) μexp=10.8 mm−1. After correction of system-induced attenuation (μCAL=1.1 mm−1), the decay rates match closely with the decay of the simulated curves: (a) μsim=3.6 mm−1 and (b) μsim=9.7 mm−1. Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO

Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. The volume-fraction dependence of the OCT attenuation coefficient, μOCT, of four different sized silica beads (mean diameter: 0.47, 0.70, 0.91, and 1.60 μm). The black dots depict the experimental data point and the error bars depict the uncertainty estimated as the standard deviation of 100 fits. The plotted curves show the calculated data. The blue dotted lines are the Mie calculations, the red dashed lines are the Mie calculations combined with Percus–Yevick formalism (Mie+PY) to include concentration-dependent scattering, and the green lines are the calculations combining Mie+PY with the EHF model to account for multiple scattering. Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO

Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. The calculated scattering anisotropy (g) of the silica beads as a function of their volume fractions. The blue dotted lines are the single, concentration-independent scattering, Mie, calculations. The red dashed lines are the single, concentration-dependent scattering calculation, where Mie theory is combined with the Percus–Yevick PCF (Mie+PY). A change in scattering anisotropy as a function of volume fraction is predicted when comparing Mie+PY (single, concentration-dependent scattering) to Mie (single, concentration-independent scattering) calculations. Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO

Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. The volume-fraction dependence of the backscattering coefficient (μB,NA). The black dots show the experimental data points and the error bars depict the standard deviation from five independent measurements. The blue dotted lines are the single, independent scattering, Mie calculations. The red dashed lines are the single, concentration-dependent scattering, Mie+PY calculations. Here, we do not include any multiple scattering, as the experimental data are taken in a thin superficial layer to minimize the contribution of multiple scattered light. A scaling factor (sf) [sfØ=[μB,NA (MIE−PY)/A2(z0)]Ø,fvMAX] is used to obtain μB,NA from A. Per particle size, we used the measurement at highest volume fraction to calculate the scaling factor. Figure Legend: From: Validation of quantitative attenuation and backscattering coefficient measurements by optical coherence tomography in the concentration-dependent and multiple scattering regime J. Biomed. Opt. 2015;20(12): doi: /1.JBO