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1

Drake, R. M., and J. E. Gordon. "Mie scattering." American Journal of Physics 53, no. 10 (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 (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 (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 assumpt
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4

Kohler, A., J. Sulé-Suso, G. D. Sockalingum, 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 (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 theoretical
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5

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

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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 (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
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7

Geiss, Andrew, and Po-Lun Ma. "NeuralMie (v1.0): an aerosol optics emulator." Geoscientific Model Development 18, no. 5 (2025): 1809–27. https://doi.org/10.5194/gmd-18-1809-2025.

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Abstract. The direct interactions of atmospheric aerosols with radiation significantly impact the Earth's climate and weather and are important to represent accurately in simulations of the atmosphere. This work introduces two contributions to enable a more accurate representation of aerosol optics in atmosphere models: (1) NeuralMie, a neural network Mie scattering emulator that can directly compute the bulk optical properties of a diverse range of aerosol populations and is appropriate for use in atmosphere simulations where aerosol optical properties are parameterized, and (2) TAMie, a fast
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8

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

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9

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

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10

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

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11

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 (1987): 795. http://dx.doi.org/10.1364/josaa.4.000795.

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12

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 (2011): 78. http://dx.doi.org/10.1364/josaa.29.000078.

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13

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

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14

Zhou, Tianze. "Research on the infrared scattering characteristics of films doped with infrared lossless nanoparticles based on mie scattering." Journal of Physics: Conference Series 2888, no. 1 (2024): 012018. http://dx.doi.org/10.1088/1742-6596/2888/1/012018.

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Abstract Recently, infrared scattering has caught people’s interest because of its stealth capabilities, heat insulation properties, polarization control, and other factors. This study specifically explores Mie scattering in the infrared spectrum, which is a well-established theory describing how light is absorbed and scattered by particles. We will analyze the periodic structure of nanoparticles made from ZnS, calculating their reflectance, transmission, and far-field scattering characteristics. Lastly, we will present scattering effect of ZnS/SEBS coating sprayed onto metal, illustrating how
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15

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 (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
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16

Prasher, Ravi S. "Mie Scattering Theory for Phonon Transport in Particulate Media." Journal of Heat Transfer 126, no. 5 (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 conv
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17

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 (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 wit
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18

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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19

Velazco, Abner, and Abel Gutarra. "Determinación del tamaño de partículas pequeñas por scattering de luz." Revista Cientifica TECNIA 27, no. 2 (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 variac
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20

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 (2012): 658–60. http://dx.doi.org/10.1109/lpt.2012.2185786.

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21

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

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22

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

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23

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

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24

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

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25

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 (2009): 1–8. http://dx.doi.org/10.1016/j.jappgeo.2008.08.008.

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26

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 (2012): 011110. http://dx.doi.org/10.1063/1.4730408.

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27

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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28

TRAVIS, KORT, and JOCHEN GUCK. "SCATTERING FROM SINGLE NANOPARTICLES: MIE THEORY REVISITED." Biophysical Reviews and Letters 01, no. 02 (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
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29

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 (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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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 sp
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31

Hamill, Colin D., Alexandria V. Johnson, and Peter Gao. "Light Scattering Measurements of KCl Particles as an Exoplanet Cloud Analog." Planetary Science Journal 5, no. 8 (2024): 186. http://dx.doi.org/10.3847/psj/ad6569.

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Abstract Salt clouds are predicted to be common on warm exoplanets, but their optical properties are uncertain. The Exoplanet Cloud Ensemble Scattering System (ExCESS), a new apparatus to measure the scattering intensity and degree of linear polarization for an ensemble of particles, is introduced here and used to study the light scattering properties of KCl cloud analogs. ExCESS illuminates particles with a polarized laser beam (532 nm) and uses a photomultiplier tube detector to sweep the plane of illumination. Scattering measurements for KCl particles were collected for three size distribut
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32

Becchetti, F. D. "The nuclear optical model and its optical-scattering analog: Mie scattering." American Journal of Physics 91, no. 8 (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 wavelengt
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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 (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 B
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34

Belozerova, Nadezhda M., Denis A. Kislov, Ilia D. Medvedev, et al. "Raman scattering from silicon resonant Mie-voids." Applied photonics 11, no. 4 (2024): 5–19. https://doi.org/10.15593/2411-4375/2024.4.01.

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The influence of Mie resonances on optical scattering processes is one of the key aspects in nanophotonics. This work is devoted to the study of Raman scattering from silicon resonant Mievoids. The enhancement of the Raman scattering signal associated with the presence of multipole resonances in these structures is experimentally shown. The results demonstrate the dependence of the optical characteristics on the geometry of the samples and confirm the potential of using Mievoids in modern nanophotonic devices. The results of numerical simulation performed by the finite element method are in go
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35

Ibrahim, Misbah, Ahmed Al Muyeed Syed, Kundu Babuya Soumik, Mehtanin Khabir Kanij, and Shafiqul Islam Md. "Study on the Absorption and Scattering Efficiencies of the Cadmium Telluride Nanowire." International Journal of Advances in Materials Science and Engineering (IJAMSE) 4, October (2015): 23–29. https://doi.org/10.5281/zenodo.3342035.

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The optical properties of cadmium telluride nanowires have been simulated using the Mie scattering coefficients. It is seen that the absorption efficiency shows multiple peaks along the spectrum due to leaky mode resonance. The nanowires showed strong polarization dependence in smaller radius. Higher angle of incidence showed a suppressing effect on lower valued peaks on absorption efficiency. Scattering efficiency showed peaks at visible spectrum from 30nm to 100nm. Transverse magnetic wave showed a more pronounced effect in scattering than transverse electric wave.
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36

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
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37

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
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38

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 pa
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39

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

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40

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
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41

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 (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 M
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42

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 (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
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43

Akyüz, Ali Özhan, and Kazım Kumaş. "A Simulation-Based Study of Static Light Scattering in Polymer Solutions: Exploring Rayleigh, Mie, Debye, and Guinier Models." Afyon Kocatepe Üniversitesi Uluslararası Mühendislik Teknolojileri ve Uygulamalı Bilimler Dergisi 8, no. 1 (2025): 1–13. https://doi.org/10.53448/akuumubd.1662307.

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This study investigated the scattering behavior of polymer particles in a solvent using a simulation-based approach. A laser source with a wavelength of 635 nm was employed, and scattering angles were calculated within the range of 0° to 175°. The refractive indices of the solvent and polymer particles were set to 1.33 (typical for water) and 1.59 (commonly observed for polymers), respectively. The radius of gyration, estimated from the hydrodynamic diameter, was taken as 58.5 nm. Four models—Rayleigh, Mie, Debye, and Guinier—were applied to analyze the scattering behavior. Rayleigh scattering
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44

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 (2020): 083112. http://dx.doi.org/10.1063/5.0015050.

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45

Kazadi Mukenga Bantu, A., T. Mabiala Masiala, E. Phuku Phuati, J. P. Mbungu Tsumbu, and P. Defrance. "Double Approach in the Investigation of Light Scattering by a Nickel Metal Cylinder." European Journal of Applied Physics 4, no. 1 (2022): 52–59. http://dx.doi.org/10.24018/ejphysics.2022.4.1.134.

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In the present work, we have investigated the light scattering from a Nickel metal cylinder under normal incidence. A double approach using the Fresnel reflectance model and Lorenz-Mie approach shows that the Fresnel model cannot follow the changes in the scattering regime when the size parameter changes. Experiments show that, even for large cylinders, the Fresnel model overestimates the effects of reflection in the forward direction. The simulation using the Lorenz-Mie formalism shows that as the size parameter changes the scattering regime changes and for size parameter lower than one the d
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46

Thinh, Cong Tran, Doan Quoc Anh Nguyen, and Thi Phuong Loan Nguyen. "Comparison of calcium carbonate and titania particles on improving color homogeneity and luminous flux of WLEDs." TELKOMNIKA Telecommunication, Computing, Electronics and Control 18, no. 5 (2020): 2690~2695. https://doi.org/10.12928/TELKOMNIKA.v18i5.13552.

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In this paper, the experiments on phosphor-converted LEDs (pc-LEDs) with a correlated color temperature (CCT) of 8500K has been conducted with the scattering enhancement particles (SEPs) to achieve the higher color uniformity and emitted luminous flux of pc-LEDs. Moreover, this paper also introduced about choosing scattering enhancement particles (SEPs), including calcium carbonate (CaCO3) and titania (TiO2), and compared these particles’ properties by adding them into the yellow Y3Al5O12:Ce3+ phosphor compounding. Afterward, the LightTools program was applied to illustrate the optical s
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47

Lu, Yuqing, Jiandong Mao, Yingnan Zhang, et al. "Simulation and Analysis of Mie-Scattering Lidar-Measuring Atmospheric Turbulence Profile." Sensors 22, no. 6 (2022): 2333. http://dx.doi.org/10.3390/s22062333.

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Based on the residual turbulent scintillation theory, the Mie-scattering lidar can measure the intensity of atmospheric turbulence by detecting the light intensity scintillation index of the laser return signal. In order to evaluate and optimize the reliability of the Mie-scattering lidar system for detecting atmospheric turbulence, the appropriate parameters of the Mie-scattering lidar system are selected and optimized using the residual turbulent scintillation theory. Then, the Fourier transform method is employed to perform the numerical simulation of the phase screen of the laser light int
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48

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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49

Geer, A. J., and F. Baordo. "Improved scattering radiative transfer for frozen hydrometeors at microwave frequencies." Atmospheric Measurement Techniques 7, no. 6 (2014): 1839–60. http://dx.doi.org/10.5194/amt-7-1839-2014.

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Abstract. To simulate passive microwave radiances in all-sky conditions requires better knowledge of the scattering properties of frozen hydrometeors. Typically, snow particles are represented as spheres and their scattering properties are calculated using Mie theory, but this is unrealistic and, particularly in deep-convective areas, it produces too much scattering in mid-frequencies (e.g. 30–50 GHz) and too little scattering at high frequencies (e.g. 150–183 GHz). These problems make it hard to assimilate microwave observations in numerical weather prediction (NWP) models, particularly in si
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50

Geer, A. J., and F. Baordo. "Improved scattering radiative transfer for frozen hydrometeors at microwave frequencies." Atmospheric Measurement Techniques Discussions 7, no. 2 (2014): 1749–805. http://dx.doi.org/10.5194/amtd-7-1749-2014.

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Abstract:
Abstract. To simulate passive microwave radiances in all-sky conditions requires better knowledge of the scattering properties of frozen hydrometeors. Typically, snow particles are represented as spheres and their scattering properties are calculated using Mie theory, but this is unrealistic and particularly in deep-convective areas, it produces too much scattering in mid frequencies (e.g. 30–50 GHz) and too little scattering at high frequencies (e.g. 150–183 GHz). These problems make it hard to assimilate microwave observations in numerical weather prediction (NWP) models, particularly in sit
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