Ping Yang

Prof. Ping Yang

Holder of the David Bullock Harris Chair, Department of Atmospheric Sciences, Texas A&M University, College Station, TX 77843, USA

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 January 2013 in Journal of the Atmospheric Sciences
Verified
Journal Article
Open access
Ping YangPing Yang
Ping Yang
LBLei Bi
Lei Bi
BBBryan A. Baum
Bryan A. Baum
KLKuo-Nan Liou
Kuo-Nan Liou
GKGeorge W. Kattawar
George W. Kattawar
BCBenjamin Cole
Benjamin Cole
A data library is developed containing the scattering, absorption, and polarization properties of ice particles in the spectral range from 0.2 to 100 μm. The properties are computed based on a combination of the Amsterdam discrete dipole approximation (ADDA), the T-matrix method, and the improved geometric optics method (IGOM). The electromagnetic edge effect is incorporated into the extinction and absorption efficiencies computed from the IGOM. A full set of single-scattering properties is provided by considering three-dimensional random orientations for 11 ice crystal habits: droxtals, prolate spheroids, oblate spheroids, solid and hollow columns, compact aggregates composed of eight solid columns, hexagonal plates, small spatial aggregates composed of 5 plates, large spatial aggregates composed of 10 plates, and solid and hollow bullet rosettes. The maximum dimension of each habit ranges from 2 to 10 000 μm in 189 discrete sizes. For each ice crystal habit, three surface roughness conditions (i.e., smooth, moderately roughened, and severely roughened) are considered to account for the surface texture of large particles in the IGOM applicable domain. The data library contains the extinction efficiency, single-scattering albedo, asymmetry parameter, six independent nonzero elements of the phase matrix (P11, P12, P22, P33, P43, and P44), particle projected area, and particle volume to provide the basic single-scattering properties for remote sensing applications and radiative transfer simulations involving ice clouds. Furthermore, a comparison of satellite observations and theoretical simulations for the polarization characteristics of ice clouds demonstrates that ice cloud optical models assuming severely roughened ice crystals significantly outperform their counterparts assuming smooth ice crystals.

28 November 2014 in Advances in Atmospheric Sciences
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Journal Article
Closed access
PDF file
Ping YangPing Yang
Ping Yang
KLKuo-Nan Liou
Kuo-Nan Liou
LBLei Bi
Lei Bi
CLChao Liu
Chao Liu
BYBingqi Yi
Bingqi Yi
BBBryan A. Baum
Bryan A. Baum

27 March 2012 in Journal of Geophysical Research: Atmospheres
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Journal Article
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HIHironobu Iwabuchi
Hironobu Iwabuchi
Ping YangPing Yang
Ping Yang
KLK. N. Liou
K. N. Liou
PMPatrick Minnis
Patrick Minnis

17 December 2018 in Atmosphere
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Journal Article
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Ping YangPing Yang
Ping Yang
SHSouichiro Hioki
Souichiro Hioki
MSMasanori Saito
Masanori Saito
CKChia-Pang Kuo
Chia-Pang Kuo
BBBryan A. Baum
Bryan A. Baum
KLKuo-Nan Liou
Kuo-Nan Liou
The current wealth of spaceborne passive and active measurements from ultraviolet to the infrared wavelengths provides an unprecedented opportunity to construct ice cloud bulk optical property models that lead to consistent ice cloud property retrievals across multiple sensors and platforms. To infer the microphysical and radiative properties of ice clouds from these satellite measurements, the general approach is to assume an ice cloud optical property model that implicitly assumes the habit (shape) and size distributions of the ice particles in these clouds. The assumption is that this ice optical property model will be adequate for global retrievals. In this review paper, we first summarize the key optical properties of individual particles and then the bulk radiative properties of their ensemble, followed by a review of the ice cloud models developed for application to satellite remote sensing. We illustrate that the random orientation condition assumed for ice particles is arguably justified for passive remote sensing applications based on radiometric measurements. The focus of the present discussion is on the ice models used by the Moderate Resolution Imaging Spectroradiometer (MODIS) and the Clouds and Earth’s Radiant Energy System (CERES) science teams. In addition, we briefly review the ice cloud models adopted by the Polarization and Directionality of the Earth’s Reflectance (POLDER) and the Himawari-8 Advanced Himawari Imager (AHI) for ice cloud retrievals. We find that both the MODIS Collection 6 ice model and the CERES two-habit model result in spectrally consistent retrievals.

28 April 2015 in Optics Express
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CZChen Zhou
Chen Zhou
Ping YangPing Yang
Ping Yang
At a wavelength corresponding to negligible electromagnetic absorption by ice, rigorous numerical simulations based on solving Maxwell’s equations show a backscattering peak associated with the phase function of randomly oriented hexagonal ice crystals. The backscattering peak, which has important implications to the interpretation of lidar observations, exists in the cases of smooth regular, smooth irregular, and roughened hexagonal ice crystals. The backscattering peak width is inversely proportional to the size parameter. The theoretical prediction of the backscattering peak is consistent with observations.

8 September 2021 in Geophysical Research Letters
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Journal Article
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MSMasanori Saito
Masanori Saito
Ping YangPing Yang
Ping Yang
Sensitivities of the backscattering properties to the microphysical properties (in particular, size and shape) of mineral dust aerosols are examined based on TAMUdust2020, a comprehensive single‐scattering property database of irregular aerosol particles. We develop the bulk mineral dust particle models based on size‐resolved particle ensembles with randomly distorted shapes and spectrally resolved complex refractive indices, which are constrained by using in situ observations reported in the literature. The light detection and ranging (lidar) ratio is more sensitive to particle shape than particle size, while the depolarization ratio depends strongly on particle size. The simulated bulk backscattering properties (i.e., the lidar ratio and the depolarization ratio) of typical mineral dust particles with effective radii of 0.5–3 µm are reasonably consistent with lidar observations made during several field campaigns. The present dust bulk optical property models are applicable to lidar‐based remote sensing of dust aerosol properties.