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manoharan-lab
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python-mie
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use pint.get_application_registry() to handle downstream unit registries
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#54:
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2456f3c
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4m 46s
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changed integrate_intensity() to return array rather than tuple
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#53:
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ec21f83
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made kd optional for integrate_intensity() and diff_scat_intensity()
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#52:
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added test for vectorization over 2D array of angles
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#51:
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4m 21s
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added test for vectorization over 2D array of angles
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#50:
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moved polarization axis to last axis to make xr.apply_ufunc() easier
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#49:
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6m 9s
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generalized broadcasting in mie special functions
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#48:
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5m 15s
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added _shift_and_pad() utility function and used throughout
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generalized _scatcoeffs_multi() to work with multidimensional m, x
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#46:
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added information on broadcasting and array shapes to module docstring
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#45:
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4m 54s
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simplified reshaping in amplitude_scattering_matrix()
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#44:
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4m 18s
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simplified integrate_intensity_complex_medium()
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#43:
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removed diff. cross-secs from output of integrate_intensity_complex_m…
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#42:
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removed cartesian option; now use phis to determine coordinate system
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#41:
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5m 7s
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changed functions to no longer use meshgrid for theta, phi
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#40:
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diff_... and integrate..._complex_medium() now take 1D thetas and phis
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#39:
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4m 22s
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allow calc_ang_scat() to take incident_vector argument
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#38:
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let calc_ang_dist() call diff_scat_intensity_complex_medium() with kd…
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#37:
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4m 34s
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split Rayleigh-Gans form factor calculation into new function
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#36:
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removed dimension checks and many reshaping operations throughout
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#35:
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changed index_ratio() and size_parameter() to always output at least 2D
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#34:
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removed unused import
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#33:
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changed _internal_coeffs() to not squeeze wavelen axis
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#32:
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changed _scatcoeffs() and all related funcs to not squeeze wavelen axis
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#31:
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changed from scipy trapezoid to np.trapezoid for integration
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#30:
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