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Journal articles on the topic 'Mie scattering'

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Published: 4 June 2021
Last updated: 8 June 2024

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1

Drake, R. M., and J. E. Gordon. "Mie scattering." American Journal of Physics 53, no. 10 (October 1985): 955–62. http://dx.doi.org/10.1119/1.14011.

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2

Du, Hong. "Mie-scattering calculation." Applied Optics 43, no. 9 (March 19, 2004): 1951. http://dx.doi.org/10.1364/ao.43.001951.

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3

Guo, Yu, Adrian Jarabo, and Shuang Zhao. "Beyond mie theory." ACM Transactions on Graphics 40, no. 6 (December 2021): 1–12. http://dx.doi.org/10.1145/3478513.3480543.

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Light scattering in participating media and translucent materials is typically modeled using the radiative transfer theory. Under the assumption of independent scattering between particles, it utilizes several bulk scattering parameters to statistically characterize light-matter interactions at the macroscale. To calculate these parameters based on microscale material properties, the Lorenz-Mie theory has been considered the gold standard. In this paper, we present a generalized framework capable of systematically and rigorously computing bulk scattering parameters beyond the far-field assumption of Lorenz-Mie theory. Our technique accounts for microscale wave-optics effects such as diffraction and interference as well as interactions between nearby particles. Our framework is general, can be plugged in any renderer supporting Lorenz-Mie scattering, and allows arbitrary packing rates and particles correlation; we demonstrate this generality by computing bulk scattering parameters for a wide range of materials, including anisotropic and correlated media.
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4

Sorensen, C. M., and D. J. Fischbach. "Patterns in Mie scattering." Optics Communications 173, no. 1-6 (January 2000): 145–53. http://dx.doi.org/10.1016/s0030-4018(99)00624-0.

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5

Kohler, A., J. Sulé-Suso, G. D. Sockalingum, M. Tobin, F. Bahrami, Y. Yang, J. Pijanka, et al. "Estimating and Correcting Mie Scattering in Synchrotron-Based Microscopic Fourier Transform Infrared Spectra by Extended Multiplicative Signal Correction." Applied Spectroscopy 62, no. 3 (March 2008): 259–66. http://dx.doi.org/10.1366/000370208783759669.

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We present an approach for estimating and correcting Mie scattering occurring in infrared spectra of single cells, at diffraction limited probe size, as in synchrotron based microscopy. The Mie scattering is modeled by extended multiplicative signal correction (EMSC) and subtracted from the vibrational absorption. Because the Mie scattering depends non-linearly on α, the product of the radius and the refractive index of the medium/sphere causing it, a new method was developed for estimating the Mie scattering by EMSC for unknown radius and refractive index of the Mie scatterer. The theoretically expected Mie contributions for a range of different α values were computed according to the formulae developed by Van de Hulst (1957). The many simulated spectra were then summarized by a six-dimensional subspace model by principal component analysis (PCA). This subspace model was used in EMSC to estimate and correct for Mie scattering, as well as other additive and multiplicative interference effects. The approach was applied to a set of Fourier transform infrared (FT-IR) absorbance spectra measured for individual lung cancer cells in order to remove unwanted interferences and to estimate ranges of important α values for each spectrum. The results indicate that several cell components may contribute to the Mie scattering.
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6

Hanaishi, Ryuji, and Kazuhisa A. Chikita. "A Study on the Blue Coloration of Ao-ike Pond, Aomori Prefecture, Japan: Formulation of a Physical Model in Terms of Radiance and Image Analyses." Applied Sciences 11, no. 19 (October 4, 2021): 9231. http://dx.doi.org/10.3390/app11199231.

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The blue coloration model of a closed pond, Ao-ike Pond, Aomori Prefecture, Japan, was formulated in terms of radiance by applying a theory of observation devices proposed by Szirmay-Kalos (2008) and Hanaishi’s reverse ray tracing method. In this model, three potential contributions to the coloration were considered; irregular reflection at the Lambertian pond bottom, density fluctuation scattering by water, and Mie scattering by suspended solids. By utilizing model formulas for these mechanisms, some parameters were determined in order to duplicate the images of the pond surface without solar shading by tree leaves above the pond surface, in addition to the images with sunbeam trajectories by solar radiations passing through tree leaves, which are emitted from the water and visible on the surface. Simulating the pictures of the pond surface and the sun-beam-image analyses revealed that the blue colorations of Ao-ike Pond are mainly produced (1) by the density fluctuation scattering of water itself and the white Mie scattering by suspended solids and (2) by the red-light absorption by water in the optical paths before and after the two scatterings. Then, the density fluctuation scattering of water and the Mie scattering by suspended solids exhibited contributions of almost equal magnitude. The contribution of irregular reflections at the pond bottom was judged to be relatively small.
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7

Kivshar, Yuri. "Mie scattering yields chiral nonlinearity." Nature Photonics 16, no. 2 (February 2022): 89–90. http://dx.doi.org/10.1038/s41566-022-00953-9.

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8

Caruthers, Jerald W. "On Rayleigh and Mie scattering." Journal of the Acoustical Society of America 130, no. 4 (October 2011): 2554. http://dx.doi.org/10.1121/1.3655229.

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9

Nelissen, Radboud, Elmer Koene, Sascha Hilgenfeldt, and Michel Versluis. "Mie scattering off coated microbubbles." Journal of the Acoustical Society of America 112, no. 5 (November 2002): 2371. http://dx.doi.org/10.1121/1.4779626.

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10

Box, Michael A., Bruce H. J. McKellar, Phil Attard, and Gary Bryant. "Sum rules for Mie scattering." Journal of the Optical Society of America A 4, no. 5 (May 1, 1987): 795. http://dx.doi.org/10.1364/josaa.4.000795.

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11

Fischer, David G., Thomas van Dijk, Taco D. Visser, and Emil Wolf. "Coherence effects in Mie scattering." Journal of the Optical Society of America A 29, no. 1 (December 7, 2011): 78. http://dx.doi.org/10.1364/josaa.29.000078.

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12

Schade, H., and Z. E. Smith. "Mie scattering and rough surfaces." Applied Optics 24, no. 19 (October 1, 1985): 3221. http://dx.doi.org/10.1364/ao.24.003221.

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13

Prasher, Ravi S. "Mie Scattering Theory for Phonon Transport in Particulate Media." Journal of Heat Transfer 126, no. 5 (October 1, 2004): 793–804. http://dx.doi.org/10.1115/1.1795243.

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Scattering theory for the scattering of phonons by particulate scatterers is developed in this paper. Recently the author introduced the generalized equation of phonon radiative transport (GEPRT) in particulate media, which included a phase function to account for the anisotropic scattering of phonons by particulate scatterer. Solution of the GEPRT showed that scattering cross section is different from the thermal transport cross-section. In this paper formulations for the scattering and transport cross section for horizontally shear (SH) wave phonon or transverse wave phonon without mode conversion is developed. The development of the theory of scattering and the transport cross section is exactly analogous to the Mie scattering theory for photon transport in particulate media. Results show that transport cross section is very different from the scattering cross section. The theory of phonon scattering developed in this paper will be useful for the predictive modeling of thermal conductivity of practical systems, such as nanocomposites, nano-micro-particle-laden systems, etc.
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14

Liu, Guigen, Yihui Wu, Kaiwei Li, Peng Hao, Ping Zhang, and Ming Xuan. "Mie Scattering-Enhanced Fiber-Optic Refractometer." IEEE Photonics Technology Letters 24, no. 8 (April 2012): 658–60. http://dx.doi.org/10.1109/lpt.2012.2185786.

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15

Gregory, Don A. "Mie scattering of growing molecular contaminants." Optical Engineering 46, no. 3 (March 1, 2007): 033602. http://dx.doi.org/10.1117/1.2715944.

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16

Cachorro, V. E., and L. L. Salcedo. "New Improvements for Mie Scattering Calculations." Journal of Electromagnetic Waves and Applications 5, no. 9 (January 1, 1991): 913–26. http://dx.doi.org/10.1163/156939391x00950.

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17

Gordon, J. E. "Simple method for approximating Mie scattering." Journal of the Optical Society of America A 2, no. 2 (February 1, 1985): 156. http://dx.doi.org/10.1364/josaa.2.000156.

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18

Xu, M., and R. R. Alfano. "More on patterns in Mie scattering." Optics Communications 226, no. 1-6 (October 2003): 1–5. http://dx.doi.org/10.1016/j.optcom.2003.08.019.

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19

Vai, Rossana, Francisco Luzón, Ursula Iturrarán-Viveros, and Francisco J. Sánchez-Sesma. "Mie elastic scattering generated by cracks." Journal of Applied Geophysics 67, no. 1 (January 2009): 1–8. http://dx.doi.org/10.1016/j.jappgeo.2008.08.008.

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20

He, Guang S., Wing-Cheung Law, Liwei Liu, Xihe Zhang, and Paras N. Prasad. "Stimulated Mie scattering in nanocrystals suspension." Applied Physics Letters 101, no. 1 (July 2, 2012): 011110. http://dx.doi.org/10.1063/1.4730408.

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21

Fiedler-Ferrari, Nelson, and Herch Moysés Nussenzveig. "Mie Scattering near the Critical Angle." Particle & Particle Systems Characterization 4, no. 1-4 (1987): 147–50. http://dx.doi.org/10.1002/ppsc.19870040130.

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22

Ladouce, Mathieu, Tarek Barakat, Bao-Lian Su, Olivier Deparis, and Sébastien R. Mouchet. "Scattering of ultraviolet light by avian eggshells." Faraday Discussions 223 (2020): 63–80. http://dx.doi.org/10.1039/d0fd00034e.

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Using Mie scattering modelling and near-UV spectrophotometric measurements of hen, duck and quail eggshells, we propose that Mie backscattering is the origin of the UV response of the eggshells of many other bird species.
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23

Zhang, Yingnan, Jiandong Mao, Juan Li, and Xin Gong. "Novel Simulation and Analysis of Mie-Scattering Lidar for Detecting Atmospheric Turbulence Based on Non-Kolmogorov Turbulence Power Spectrum Model." Entropy 24, no. 12 (December 1, 2022): 1764. http://dx.doi.org/10.3390/e24121764.

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The Mie-scattering lidar can detect atmospheric turbulence intensity by using the return signals of Gaussian beams at different heights. The power spectrum method and Zernike polynomial method are used to simulate the non-Kolmogorov turbulent phase plate, respectively, and the power spectrum method with faster running speed is selected for the subsequent simulation. In order to verify the possibility of detecting atmospheric turbulence by the Mie-scattering lidar, some numerical simulations are carried out. The power spectrum method is used to simulate the propagation of the Gaussian beam from the Mie-scattering lidar in a vertical path. The propagation characteristics of the Gaussian beam using a non-Kolmogorov turbulence model are obtained by analyzing the intensity distribution and spot drift effect. The simulation results show that the scintillation index of simulation is consistent with the theoretical value trend, and the accuracy is very high, indicating that the method of atmospheric turbulence detection using Mie-scattering lidar is effective. The simulation plays a guiding role for the subsequent experimental platform construction and equipment design.
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24

TRAVIS, KORT, and JOCHEN GUCK. "SCATTERING FROM SINGLE NANOPARTICLES: MIE THEORY REVISITED." Biophysical Reviews and Letters 01, no. 02 (April 2006): 179–207. http://dx.doi.org/10.1142/s1793048006000136.

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Recent intense interest in nanoparticle materials and nanoparticle-based contrast enhancement agents for biophysical applications gives new relevance to Mie scattering theory in its original context of application. The Mie theory still provides the most exact treatment of scattering from single nanoparticles of the noble metals. When recast in terms of modern electrodynamic formalism, the theory provides a concise closed-form representation for the scattered fields and also serves as a vehicle to elaborate the formal electrodynamic technique. The behavior of the Debye truncation condition for the multipole expansion is illustrated with numerical examples, clearly showing the features of the transition between the Rayleigh, dipole and higher order multipole approximations for the scattered fields. The classical Mie theory is an approximation in that only the transverse field components are included in the calculation. Extensions to the classical theory which include the effects of longitudinal fields are discussed and illustrated numerically. The example of scattering from multilayer composite particles is used to examine the feasibility of engineering spectral features of the scattering cross-section to target the requirements of specific applications.
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25

FU, JIANWEI, GUOTAO QUAN, and HUI GONG. "A SIMPLE METHOD FOR PREDICTION OF THE REDUCED SCATTERING COEFFICIENT IN TISSUE-SIMULATING PHANTOMS." Journal of Innovative Optical Health Sciences 03, no. 01 (January 2010): 53–59. http://dx.doi.org/10.1142/s1793545810000770.

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This paper proposes a method for predicting the reduced scattering coefficients of tissue-simulating phantoms or the desired amount of scatters for producing phantoms according to Mie scattering theory without measurements with other instruments. The concentration of the scatters TiO 2 particles is determined according to Mie theory calculation and added to transparent host epoxy resin to produce phantoms with different reduced scattering coefficients. Black India Ink is added to alter the absorption coefficients of the phantoms. The reduced scattering coefficients of phantoms are measured with single integrating sphere system. The results show that the measurements are in direct proportion to the concentration of TiO 2 and have identical with Mie theory calculation at multiple wavelengths. The method proposed can accurately determine the concentration of scatters in the phantoms to ensure the phantoms are qualified with desired reduced scattering coefficients at specified wavelength. This investigation should be possible to manufacture the phantom simply in reasonably accurate for evaluation of biomedical optical imaging systems.
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26

Becchetti, F. D. "The nuclear optical model and its optical-scattering analog: Mie scattering." American Journal of Physics 91, no. 8 (August 1, 2023): 637–43. http://dx.doi.org/10.1119/5.0152813.

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The methods devised by Gustav Mie in 1908 to explain the scattering of electromagnetic waves have a close analogy with quantum-mechanical models developed many years later to describe nuclear scattering. In particular, these models use either a complex index of refraction or a complex nuclear scattering potential to account for attenuation caused by non-elastic scattering. We briefly outline the historical development of these models and give examples illustrating the close analogy between them, their parameters, and the resulting scattering. In both models, the ratio of the incident wavelength to the object size, λ/D, can be determined from the scattering characteristics, allowing the extraction of microscopic particle dimensions. This close analogy allows students to simulate accelerator-based nuclear scattering experiments with table-top optical-scattering experiments.
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27

Pappas, Dimitri, Tiffany L. Correll, Nathan C. Pixley, Benjamin W. Smith, and J. D. Winefordner. "Detection of Mie Scattering Using a Resonance Fluorescence Monochromator." Applied Spectroscopy 56, no. 9 (September 2002): 1237–40. http://dx.doi.org/10.1366/000370202760295502.

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The use of a resonance fluorescence monochromator (RFM) is described as a method for detecting Mie scatter. The detector has a spectral resolution limited by the atomic vapor used in the system (400 MHz for cesium). The RFM is used to detect Mie scatter from a particulate suspension, and deconvolution methods are used to extract the Mie scatter spectrum from the instrument response. The Mie scattering linewidth (140 MHz) is close to the literature value (100 MHz for air). Methods to reduce the linewidth of atomic vapor filters are briefly described.
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28

Velazco, Abner, and Abel Gutarra. "Determinación del tamaño de partículas pequeñas por scattering de luz." Revista Cientifica TECNIA 27, no. 2 (April 4, 2018): 27. http://dx.doi.org/10.21754/tecnia.v27i2.172.

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En este trabajo se describe el diseño y la construcción de un sistema para medir la distribución angular del scattering de luz de micro esferas dieléctricas suspendidas en agua, usando un láser como fuente de luz. El trabajo cubre el desarrollo de un sistema de detección óptico para mejorar la relación señal ruido. Reportamos medidas experimentales de scattering de luz de suspensiones coloidales de esferas de látex con diámetros nominales de 0,49 y 1,03 µm, y un coeficiente de variación de 3%. Se utilizaron dos láseres de diferentes longitudes de onda, 632,8 y 532,0 nm, para observar la variación de la distribución angular de scattering. Los resultados experimentales fueron comparados con distribuciones de scattering angular generadas por la teoría de Mie para determinar el tamaño de partícula. Los diámetros obtenidos fueron 0,49 y 0,95 µm con una incertidumbre relativa de 6,1 y 5,3%, respectivamente. Palabras clave.- Scattering de luz, teoría de Mie, micropartículas de latex. ABSTRACT In this work, we describe the design and construction of a system to measure the angular light scattering distribution from small dielectric spheres suspended in water, using a laser as the light source. It also covers the development of an optical detection system to improve the signal‐to‐noise ratio. We report on the experimental measurements of light scattering from colloidal suspensions of latex spheres with nominal diameters of 0.49 and 1.03 µm and a coefficient of variation of 3%. Two lasers with different wavelengths (632.8 and 532.0 nm) were used to observe the variation of the angular scattering distribution. The experimental results were then compared with angular scattering distributions generated from Mie theory, in order to determine the particle size. We obtained diameters of 0.49 and 0.95 µm, with a relative accuracy of 6.1 and 5.3%, respectively. Keywords.- Light scattering, Mie theory, latex microparticles.
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29

Ogura, Hisanao, and Nobuyuki Takahashi. "Scattering of waves from a random spherical surface—Mie scattering." Journal of Mathematical Physics 31, no. 1 (January 1990): 61–75. http://dx.doi.org/10.1063/1.529029.

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30

Konevskikh, Tatiana, Rozalia Lukacs, Reinhold Blümel, Arkadi Ponossov, and Achim Kohler. "Mie scatter corrections in single cell infrared microspectroscopy." Faraday Discussions 187 (2016): 235–57. http://dx.doi.org/10.1039/c5fd00171d.

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Strong Mie scattering signatures hamper the chemical interpretation and multivariate analysis of the infrared microscopy spectra of single cells and tissues. During recent years, several numerical Mie scatter correction algorithms for the infrared spectroscopy of single cells have been published. In the paper at hand, we critically reviewed existing algorithms for the correction of Mie scattering and suggest improvements. We developed an iterative algorithm based on Extended Multiplicative Scatter Correction (EMSC), for the retrieval of pure absorbance spectra from highly distorted infrared spectra of single cells. The new algorithm uses the van de Hulst approximation formula for the extinction efficiency employing a complex refractive index. The iterative algorithm involves the establishment of an EMSC meta-model. While existing iterative algorithms for the correction of resonant Mie scattering employ three independent parameters for establishing a meta-model, we could decrease the number of parameters from three to two independent parameters, which reduced the calculation time for the Mie scattering curves for the iterative EMSC meta-model by a factor of 10. Moreover, by employing the Hilbert transform for evaluating the Kramers–Kronig relations based on a FFT algorithm in Matlab, we further improved the speed of the algorithm by a factor of 100. For testing the algorithm we simulate distorted apparent absorbance spectra by utilizing the exact theory for the scattering of infrared light at absorbing spheres, taking into account the high numerical aperture of infrared microscopes employed for the analysis of single cells and tissues. In addition, the algorithm was applied to measured absorbance spectra of single lung cancer cells.
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31

Powers, S. W., E. P. Warner, G. Byun, and K. T. Lowe. "Auto-Processing Of Filtered Rayleigh Scattering Images Including Mie And Background Scattering Contributions." Proceedings of the International Symposium on the Application of Laser and Imaging Techniques to Fluid Mechanics 20 (July 11, 2022): 1–22. http://dx.doi.org/10.55037/lxlaser.20th.14.

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Filtered Rayleigh scattering (FRS) is a non-intrusive, optical-based technique that allows for simultaneous, time-averaged, measurements of three-component velocity, static temperature, and static pressure. The method of post-processing the raw images to get these variables is a non-trivial task. The post-processing scheme starts with building a model to generate simulated spectra given known velocity, temperature, and pressure values which can be iterated upon. The model also includes Mie scattering and background scattering contributions that must be taken into account. This iteration scheme allows for the simulated spectra to be matched to the experimental spectra to back out the desired flow variables. This iteration process can be lengthy and so it is important to make spectrum generation/iteration as fast as possible. This is done through the use of support vector spectrum approximation (SVSA), which is a machine learning algorithm, as well as a multivariable minimum error solver based on the least-squares fit between the simulated data and the experimental data. To prove the methodology, simulated results were first compared at different signal-to-noise ratios to determine the expected uncertainty at each SNR level. It was shown that to achieve an error of less than 1\% in all variables (velocity, static temperature, Mie intensity ratio, and background intensity ratio), the SNR must be near 40dB. This kind of SNR level is generally not expected in an experiment. Therefore, a representative experiment was conducted which included Mie and background scattering contributions. It was shown that manually processed data was capable of achieving velocity results that were within 2\% of the probe data. No other variables were achieved. The auto-processing scheme was able to achieve an error of approximately 2.5\% in velocity when compared to probe data. It was also capable of providing static temperature, Mie intensity ratio, and background intensity ratio values. The manual iteration results took several days to achieve while the auto-processing took about an hour. It is clear that this methodology is capable of automatically processing images from experiments with Mie and background scattering contributions while saving time.
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32

Olivares, Ignacio E., and P. Carrazana. "Mie scattering revisited: Study of bichromatic Mie scattering of electromagnetic waves by a distribution of spherical particles." Review of Scientific Instruments 91, no. 8 (August 1, 2020): 083112. http://dx.doi.org/10.1063/5.0015050.

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33

Ustimenko, N., D. Kornovan, K. V. Baryshnikova, A. B. Evlyukhin, and M. Petrov. "Application of Born series for modeling of Mie-resonant nanostructures." Journal of Physics: Conference Series 2015, no. 1 (November 1, 2021): 012161. http://dx.doi.org/10.1088/1742-6596/2015/1/012161.

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Abstract Born series formalism is a widely-used approach to solve a scattering problem in quantum mechanics and optics, including a problem of electromagnetic scattering on the ensembles of Mie-resonant nanoparticles. In the latter case, the Born series formalism can be used when the electromagnetic coupling between nanoparticles is weak. This can be violated near the multipole Mie-resonance of the nanoparticle. In this work, we analyze the applicability of the Born series approach for modeling the resonant optical response of Mie-nanoparticle ensembles and formulate quantitative criteria of Born series convergence and, subsequently, the applicability of this approach.
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34

LYU Yi-ying, 吕依颖, 高. 珊. GAO Shan, and 徐庆君 XU Qing-jun. "Scattering Characteristics of C@H2O Composite Particle Based on Mie Light Scattering Theory." Chinese Journal of Luminescence 40, no. 3 (2019): 298–303. http://dx.doi.org/10.3788/fgxb20194003.0298.

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35

Lin, Hong, Xin Min Wang, Chuan Lin Zhou, and Wei Zhong Li. "Study of Oceanic Suspended Particles Density Detecting Technology Based on Mie Scattering Theory." Applied Mechanics and Materials 192 (July 2012): 425–29. http://dx.doi.org/10.4028/www.scientific.net/amm.192.425.

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A new technology about ocean suspended particles density detecting by Mie scattering theory is proposed. This technology is based on analyzing and studying the transmission characteristics of the laser in the seawater. Based on Mie scattering theory, the optical scattering characteristics of oceanic suspended particles is researched, and a new method of calculating the scattering coefficient and backward scattering ratio is putted forward. By detecting the laser scattering signal under the seawater, the density information of ocean suspended particles can be gain and detect. A ocean suspended particles density detecting model based on airborne lidar system is firstly established through analyzing the absorbing and scattering characteristics of the suspended particles. By simulating and calculating, it is proved that the technology can detect and monitor the density of ocean suspended particles effectively, and therefore it can predict the density change of ocean suspended particles also.
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36

Hu, S., L. Liu, T. C. Gao, T. Zhang, and M. Chen. "A SCATTERING SIMULATION MODEL FOR NONSPHERICAL AEROSOL PARTICLES BASED ON PARALLEL FDTD SCHEME." ISPRS - International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences XLII-3/W9 (October 25, 2019): 71–76. http://dx.doi.org/10.5194/isprs-archives-xlii-3-w9-71-2019.

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Abstract. In order to simulate the scattering properties of nonspherical aerosol particles in visible and near infrared band precisely and efficiently, a scattering computation model for aerosol particles based on parallel FDTD (Finite Difference Time Domain) is developed. The basic principle of FDTD is introduced, and a new parallel computation scheme for FDTD is proposed, and is realized by MPI repeated non-blocking communication technique. The FDTD scattering model is validated against Lorenz-Mie theory and T Matrix method. Simulation results show that, the scattering properties obtained parallel FDTD scattering model are qualitatively in good agreement with the T matrix method and Lorenz-Mie theory, validating the accuracy of our model. The relative simulation error of Mueller is slightly larger in forward scattering directions than that in backward directions for particles with small size parameter, while for large particles, the result is opposite.
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37

Mukai, Sonoyo, Tadashi Mukai, and Sen Kikuchi. "Scattering Properties of Cometary Dust Based on Polarimetric Data." International Astronomical Union Colloquium 126 (1991): 249–52. http://dx.doi.org/10.1017/s0252921100066884.

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AbstractReferring to the dust model in Mukai and Mukai(1990), where the scattering by large rough particles and Mie scattering by small particles are taken into account, a phase function of linear polarization of several comets is examined, especially in a region of phase angles α near a maximum polarization. A lower maximum polarization observed in comet Austin(1989c1) than those in comets West(1975n) and P/Halley leads a speculation that a mixing ratio of rough scattering to Mie scattering in comet Austin increases from a sun-comet distance r of 0.6 AU to 1.2 AU. This implies that a shortage of large particles in comet Austin occured in r <1 AU.
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38

Emran, A., and V. F. Chevrier. "Uncertainty in Grain Size Estimations of Volatiles on Trans-Neptunian Objects and Kuiper Belt Objects." Astronomical Journal 163, no. 5 (April 5, 2022): 196. http://dx.doi.org/10.3847/1538-3881/ac559f.

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Abstract We analyze the uncertainty in grain size estimation of pure methane (CH4) and nitrogen saturated with methane (N2:CH4) ices, the most abundant volatile materials on trans-Neptunian objects (TNOs) and Kuiper Belt objects (KBOs). We compare the single scattering albedo, which determines the grain size estimation of outer solar system regolith, of these ices using the Mie scattering model and two other Hapke approximations (Hapke 1993) in radiative transfer scattering models (RTMs) at near-infrared (NIR) wavelengths (1–5 μm). The equivalent slab (Hapke slab) approximation model predicts results much closer to Mie scattering over the NIR wavelengths at a wide range of grain sizes. In contrast, even though the internal scattering model predicts an approximate particle diameter close to the Mie model for particles with a 10 μm radii, it exhibits higher discrepancies in the predicted estimation for larger grain sizes (e.g., 100 and 1000 μm radii). Owing to the Rayleigh effect on single-scattering properties, neither Hapke approximate models could predict an accurate grain size estimation for the small particles (radii ≤5 μm). We recommend that future studies should favor the Hapke slab approximation when employing RTMs for estimating grain sizes of the vast number of TNOs and KBOs in the outer solar system.
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39

Shen, Fei, Ning An, Yifei Tao, Hongping Zhou, Zhaoneng Jiang, and Zhongyi Guo. "Anomalous forward scattering of gain-assisted dielectric shell-coated metallic core spherical particles." Nanophotonics 6, no. 5 (December 9, 2016): 1063–72. http://dx.doi.org/10.1515/nanoph-2016-0141.

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AbstractWe have investigated the scattering properties of an individual core-shell nanoparticle using the Mie theory, which can be tuned to support both electric and magnetic modes simultaneously. In general, the suppression of forward scattering can be realized by the second Kerker condition. Here, a novel mechanism has to be adopted to explain zero-forward scattering, which originates from the complex interactions between dipolar and quadrupolar modes. However, for lossy and lossless core-shell spherical nanoparticles, zero-forward scattering can never be achieved because the real parts of Mie expansion coefficients are always positive. By adding proper gain in dielectric shell, zero-forward scattering can be found at certain incident wavelengths, which means that all electric and magnetic responses in Mie scattering can be counteracted totally in the forward direction. In addition, if the absolute values of dipolar and quadrupolar terms are in the same order of magnitude, the local scattering minimum and maximum can be produced away from the forward and backward directions due to the interacting effect between the dipolar and quadrupolar terms. Furthermore, by adding suitable gain in shell, super-forward scattering can also be realized at certain incident wavelengths. We also demonstrated that anomalously weak scattering or superscattering could be obtained for the core-shell nanoparticles with suitable gain in shell. In particular, for such a choice of suitable gain in shell, we can obtain zero-forward scattering and anomalously weak scattering at the same wavelength as well as super-forward scattering at another wavelength. These features may provide new opportunities for cloaking, plasmonic lasers, optical antennas, and so on.
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40

Fischer, Andreas. "Imaging Flow Velocimetry with Laser Mie Scattering." Applied Sciences 7, no. 12 (December 13, 2017): 1298. http://dx.doi.org/10.3390/app7121298.

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41

Rother, T., and K. Schmidt. "The Discretized MIE-Formalism for Electromagnetic Scattering." Progress In Electromagnetics Research 17 (1997): 91–183. http://dx.doi.org/10.2528/pier97021000.

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42

Ohnoutek, Lukas, Ji-Young Kim, Jun Lu, Ben J. Olohan, Dora M. Răsădean, G. Dan Pantoș, Nicholas A. Kotov, and Ventsislav K. Valev. "Third-harmonic Mie scattering from semiconductor nanohelices." Nature Photonics 16, no. 2 (January 13, 2022): 126–33. http://dx.doi.org/10.1038/s41566-021-00916-6.

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43

Matsuyama, Tatsushi. "Derivation of Mie Theory of Light Scattering." Journal of the Society of Powder Technology, Japan 43, no. 2 (2006): 115–24. http://dx.doi.org/10.4164/sptj.43.115.

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44

Hightower, R. L., and C. B. Richardson. "Resonant Mie scattering from a layered sphere." Applied Optics 27, no. 23 (December 1, 1988): 4850. http://dx.doi.org/10.1364/ao.27.004850.

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45

Guerra, R., and J. T. Mendonça. "Mie and Debye scattering in dusty plasmas." Physical Review E 62, no. 1 (July 1, 2000): 1190–201. http://dx.doi.org/10.1103/physreve.62.1190.

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46

Lange, Benjamin, and Sergio R. Aragón. "Mie scattering from thin anisotropic spherical shells." Journal of Chemical Physics 92, no. 8 (April 15, 1990): 4643–50. http://dx.doi.org/10.1063/1.457731.

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47

Yilmaz, Suleyman, Amirullah M. Mamedov, Mehriban Yusufova, and Faruk Karadag. "Mie Scattering and Domain Structure of Ferroelectrics." Ferroelectrics 270, no. 1 (January 2002): 315–20. http://dx.doi.org/10.1080/713716147.

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48

Rybin, M. V., I. S. Sinev, K. B. Samusev, and M. F. Limonov. "Cascades of Fano resonances in Mie scattering." Physics of the Solid State 56, no. 3 (March 2014): 580–87. http://dx.doi.org/10.1134/s1063783414030263.

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49

Scholz, S. M., R. Vacassy, J. Dutta, H. Hofmann, and M. Akinc. "Mie scattering effects from monodispersed ZnS nanospheres." Journal of Applied Physics 83, no. 12 (June 15, 1998): 7860–66. http://dx.doi.org/10.1063/1.367961.

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50

Gershon, T. S., N. N. Lal, J. J. Baumberg, and J. L. MacManus-Driscoll. "Tunable Mie Scattering from Electrodeposited Cu2O Nanoparticles." Journal of The Electrochemical Society 159, no. 12 (2012): D747—D749. http://dx.doi.org/10.1149/2.069212jes.

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