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Original Articles

Identification and particle sizing of submicron mineral dust by using complex forward-scattering amplitude data

ORCID Icon, ORCID Icon & ORCID Icon
Pages 609-622 | Received 16 Dec 2021, Accepted 20 Mar 2022, Published online: 07 Apr 2022

Figures & data

Figure 1. Schematic diagram of our SPES instrument with an illustration of the interferometric detection of scattered wave from each particle in forward direction.

Figure 1. Schematic diagram of our SPES instrument with an illustration of the interferometric detection of scattered wave from each particle in forward direction.

Figure 2. Scatterplot of [ImS22]sc versus ReS22 for polystyrene spheres measured by the SPES instruments. The black dots indicate single-particle data. The red-filled circles with error bars indicate the median and 10th–90th percentile ranges of single-particle data for each particle size. The blue-filled circles with error bars indicate the theoretical values and their uncertainty ranges for each particle size. The uncertainty ranges of the theoretical values were computed from the expanded uncertainty (k = 2) of each particle size specified in the sample datasheet.

Figure 2. Scatterplot of [ImS22]sc versus ReS22 for polystyrene spheres measured by the SPES instruments. The black dots indicate single-particle data. The red-filled circles with error bars indicate the median and 10th–90th percentile ranges of single-particle data for each particle size. The blue-filled circles with error bars indicate the theoretical values and their uncertainty ranges for each particle size. The uncertainty ranges of the theoretical values were computed from the expanded uncertainty (k = 2) of each particle size specified in the sample datasheet.

Table 1. List of samples.

Figure 3. Representative TEM images for each of the (a) synthetic and (b) natural samples. In (b), four elemental mappings are shown for each TEM image. The TEM images were obtained using a 120-kV TEM (JEM-1400, JEOL) and the elemental mappings were measured using an energy-dispersive X-ray spectrometer (EDS, Oxford Instruments) with scanning TEM mode (STEM-EDS).

Figure 3. Representative TEM images for each of the (a) synthetic and (b) natural samples. In (b), four elemental mappings are shown for each TEM image. The TEM images were obtained using a 120-kV TEM (JEM-1400, JEOL) and the elemental mappings were measured using an energy-dispersive X-ray spectrometer (EDS, Oxford Instruments) with scanning TEM mode (STEM-EDS).

Figure 4. Scatter plots of S22 data points for the individual samples listed in .

Figure 4. Scatter plots of S22 data points for the individual samples listed in Table 1.

Figure 5. Density plots of S22 data points for natural dust samples. The solid lines indicate the traces of median values of [ImS22]sc as a function of ReS22 for each synthetic sample. Because the S22 data points for hematite show two distinct clusters (), we separated the hematite data into two clusters using a boundary line (y = 0.95x – 0.02) and then computed the trace for each cluster.

Figure 5. Density plots of S22 data points for natural dust samples. The solid lines indicate the traces of median values of [ImS22]sc as a function of ReS22 for each synthetic sample. Because the S22 data points for hematite show two distinct clusters (Figure 4b), we separated the hematite data into two clusters using a boundary line (y = 0.95x – 0.02) and then computed the trace for each cluster.

Figure 6. Clustering results of S22 data points for natural dust samples. For each sample, the (a) Boundary and (b) HDBSCAN methods were applied to the 15,000 raw data points. The black solid lines in (a) indicate the boundary curve (y = 0.65x1.4 + 0.008). The blue solid lines with open circles indicate the principal curves for the silicate clusters, wherein the open circles indicate the 0th, 10th, …, 90th, 98th, and 100th percentiles of the arc-length coordinate of the S22 data points. The data points with the largest 2% |S22| values were removed before the principal curve fitting to avoid an overfitting issue. The data number of each cluster is denoted in the legend. The total number of data points shown in each figure is less than 15,000 because of trimming of the raw data points near the origin.

Figure 6. Clustering results of S22 data points for natural dust samples. For each sample, the (a) Boundary and (b) HDBSCAN methods were applied to the 15,000 raw data points. The black solid lines in (a) indicate the boundary curve (y = 0.65x1.4 + 0.008). The blue solid lines with open circles indicate the principal curves for the silicate clusters, wherein the open circles indicate the 0th, 10th, …, 90th, 98th, and 100th percentiles of the arc-length coordinate of the S22 data points. The data points with the largest 2% |S22| values were removed before the principal curve fitting to avoid an overfitting issue. The data number of each cluster is denoted in the legend. The total number of data points shown in each figure is less than 15,000 because of trimming of the raw data points near the origin.

Figure 7. Bar plots of log10m(D|Ml) values for the silicate cluster. The MAP estimate of the complex refractive index mMAP = mr + imi is also shown on the top of each bar plot.

Figure 7. Bar plots of −log10m(D|Ml) values for the silicate cluster. The MAP estimate of the complex refractive index mMAP = mr + imi is also shown on the top of each bar plot.

Table 2. The effective refractive indices of the silicate clusters estimated according to the Bayesian inversion method.

Figure 8. Retrieved particle-size distributions for the silicate cluster of each dust sample. For comparison, also shown by solid lines are the retrieved particle-size distributions by elastic light scattering approaches that measure only either |S22(0°)| or ImS22(0°), assuming m = 1.56 + 0i to be a typical refractive index value for single crystals of clay minerals.

Figure 8. Retrieved particle-size distributions for the silicate cluster of each dust sample. For comparison, also shown by solid lines are the retrieved particle-size distributions by elastic light scattering approaches that measure only either |S22(0°)| or ImS22(0°), assuming m = 1.56 + 0i to be a typical refractive index value for single crystals of clay minerals.

Figure B1. Scatter plots of the synthetic data that were classified by the (a) Boundary and (b) HDBSCAN methods. The black solid and black dashed lines in (a) represent the boundary curves for the curve method. Each of the blue solid lines with open circles indicates the principal curve for each silicate cluster.

Figure B1. Scatter plots of the synthetic data that were classified by the (a) Boundary and (b) HDBSCAN methods. The black solid and black dashed lines in (a) represent the boundary curves for the curve method. Each of the blue solid lines with open circles indicates the principal curve for each silicate cluster.

Figure B2. Number of data points in the silicate cluster for the synthetic data. Contributions to the number of data points in the silicate cluster from different components are shown. The red-filled circles indicate the original number of data points in the silicate cluster determined for each dust sample.

Figure B2. Number of data points in the silicate cluster for the synthetic data. Contributions to the number of data points in the silicate cluster from different components are shown. The red-filled circles indicate the original number of data points in the silicate cluster determined for each dust sample.
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