Wai Chong Fu’s research while affiliated with UNSW Sydney and other places

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Publications (2)


Scattering of a plane wave by a collinear array of scattering elements.
Typical θ − ϕ plot to illustrate ring-shaped contours representing different Bragg orders. The darker shades indicate regions representative of positive Bragg orders ( m > 0 ) and vice-versa. The contours separating the dark and light shaded regions represent points that satisfy Snell’s law of refraction.
Relationship between ϕ, θ and α, where (a) ϕ < 180 ° and θ < 180 ° − ϕ ; (b) ϕ < 180 ° and θ > 180 ° − ϕ ; (c) ϕ > 180 ° and θ < 540 ° − ϕ ; (d) ϕ > 180 ° and θ > 540 ° − ϕ .
Comparison of θ − ϕ plots generated using Kurusingal and Pennypacker approaches for the spacing factor ( a < 0.5 ) : (a) θ − ϕ plots using the Kurusingal approach, (b) θ − ϕ plots using the Purcell and Pennypacker iterative approach, and (c) plot of maximum pixel-wise relative error between the pair of θ − ϕ plots against spacing factor a.
(a) θ − ϕ plots showing diffraction contours (rings) obtained using a = 5 , N = 2 , λ = 1 e – 6   m , n = 1.2 , r 0 = 0.1   m ; (a1)–(a3) correspond to g = − 0.3 , g = 0 , and g = 0.3 . The intensities are represented by a color scale with red and blue (top and bottom of scale in print) corresponding to the maxima and minima, respectively. (b) Intensity variation along the contour representing θ − ϕ pairs that satisfy Snell’s law of refraction for a = 5 , N = 10 , λ = 1 e – 6   m , n = 1.2 . Panels (b1)–(b3) correspond to g = − 0.3 , g = 0 , and g = 0.3 , respectively. The curves shown in each panel correspond to different far-field distances, expressed as multiples of the array length ( L ) .

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Anisotropic scattering of discrete particle arrays
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April 2010

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18 Reads

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2 Citations

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Wai Chong Fu

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Far-field intensities of light scattered from a linear centro-symmetric array illuminated by a plane wave of incident light are estimated at a series of detector angles. The intensities are computed from the superposition of E-fields scattered by the individual array elements. An average scattering phase function is used to model the scattered fields of individual array elements. The nature of scattering from the array is investigated using an image ( θ − ϕ plot) of the far-field intensities computed at a series of locations obtained by rotating the detector angle from 0° to 360°, corresponding to each angle of incidence in the interval [0° 360°]. The diffraction patterns observed from the θ − ϕ plot are compared with those for isotropic scattering. In the absence of prior information on the array geometry, the intensities corresponding to θ − ϕ pairs satisfying the Bragg condition are used to estimate the phase function. An algorithmic procedure is presented for this purpose and tested using synthetic data. The relative error between estimated and theoretical values of the phase function is shown to be determined by the mean spacing factor, the number of elements, and the far-field distance. An empirical relationship is presented to calculate the optimal far-field distance for a given specification of the percentage error.

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Scattering of a plane wave by a collinear array of scattering centers.
AO intensity ( I ac ) as a function of detector angle ( θ ) for m opt = 0 . The insets show the time variation of intensity [ Δ I ( t ) ] corresponding to different θ values. The parameters used are a = 0.1 , ϕ = 30 ° , n 0 = 1.2 , r 0 = 0.1 m , λ = 1 × 10 − 6   m , λ s = 1 × 10 − 3   m , and N = 40 . (a) AO intensity due to translation of elements ( A 0 = 1 × 10 − 9   m ) ; (b) AO intensity due to variations in refractive index ( C = 1 × 10 − 4 ) .
Acousto-optic modulation of a point-scatterer array

March 2010

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11 Reads

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1 Citation

Acoustic modulation of light scattering from a linear centrosymmetric array is analyzed by considering far-field contributions due to optoelastic (OE) effect and acoustically induced translation of the array elements. The modulated light intensity is shown to vary sinusoidally at the acoustic frequency when the physical constants representative of the above effects are within ranges of their physical limits. The OE and translation components of the acousto-optic (AO) signal are shown to be in phase quadrature, each exhibiting a double-sided maxima when expressed as a function of the detector angle.

Citations (1)


... For the Fe 3 O 4 nanospheres (Figure 3a,b), the optical transmittance decreased when magnetically switching the chain orientation from 90 -90 to 90 -0 and finally 0 . According to the theoretical calculations in the literature, [16] the intensity of the scattered light is angle-dependent when a plane wave of incident light is illuminated on a linear array of nanospheres, and the mean distance between the nanospheres is less than half of the incident wavelength. The linear array of nanospheres exhibits lower transmittance when it is oriented parallel rather than perpendicular to the incidence of light. ...

Reference:

Dynamic Tuning of Optical Transmittance of One‐Dimensional Colloidal Assemblies of Magnetic Nanostructures
Anisotropic scattering of discrete particle arrays