varying the azimuth φ during the modeled by the following expressio gðθÞ = Z2π 0 Z∞ 0 Z∞ −∞ Iðz; α; φÞρ Ω where fðzÞ is the density of fluoro volved by the emission point spread the laser beam profile of divergenc describes the intensity of the electr depth z, the incidence angle α, and A B C D Fig. 2. Experimental validation of the m of the system designed to create a slope of the maximum intensity projection of im TIRF illumination. (Scale bar: 5 μm.) The ev illumination angle θ of two selected bead sponding fitting theoretical model (cont depth (respectively 10 and 89 nm). (D) Dep fitting the theoretical TIRF model (in red) estimated by fitting a Gaussian model in t [Boulanger et al. 2014] Single-molecule fluorescence (3-D) Recover pointwise sources from noisy low-resolution observations.
varying the azimuth φ during the modeled by the following expressio gðθÞ = Z2π 0 Z∞ 0 Z∞ −∞ Iðz; α; φÞρ Ω where fðzÞ is the density of fluoro volved by the emission point spread the laser beam profile of divergenc describes the intensity of the electr depth z, the incidence angle α, and A B C D Fig. 2. Experimental validation of the m of the system designed to create a slope of the maximum intensity projection of im TIRF illumination. (Scale bar: 5 μm.) The ev illumination angle θ of two selected bead sponding fitting theoretical model (cont depth (respectively 10 and 89 nm). (D) Dep fitting the theoretical TIRF model (in red) estimated by fitting a Gaussian model in t [Boulanger et al. 2014] Single-molecule fluorescence (3-D) Recover pointwise sources from noisy low-resolution observations. Mixture estimation <latexit 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varying the azimuth φ during the modeled by the following expressio gðθÞ = Z2π 0 Z∞ 0 Z∞ −∞ Iðz; α; φÞρ Ω where fðzÞ is the density of fluoro volved by the emission point spread the laser beam profile of divergenc describes the intensity of the electr depth z, the incidence angle α, and A B C D Fig. 2. Experimental validation of the m of the system designed to create a slope of the maximum intensity projection of im TIRF illumination. (Scale bar: 5 μm.) The ev illumination angle θ of two selected bead sponding fitting theoretical model (cont depth (respectively 10 and 89 nm). (D) Dep fitting the theoretical TIRF model (in red) estimated by fitting a Gaussian model in t [Boulanger et al. 2014] Single-molecule fluorescence (3-D) Recover pointwise sources from noisy low-resolution observations. Perceptron with 1 hidden layer <latexit 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Mixture estimation <latexit 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<latexit 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varying the azimuth φ during the modeled by the following expressio gðθÞ = Z2π 0 Z∞ 0 Z∞ −∞ Iðz; α; φÞρ Ω where fðzÞ is the density of fluoro volved by the emission point spread the laser beam profile of divergenc describes the intensity of the electr depth z, the incidence angle α, and A B C D Fig. 2. Experimental validation of the m of the system designed to create a slope of the maximum intensity projection of im TIRF illumination. (Scale bar: 5 μm.) The ev illumination angle θ of two selected bead sponding fitting theoretical model (cont depth (respectively 10 and 89 nm). (D) Dep fitting the theoretical TIRF model (in red) estimated by fitting a Gaussian model in t [Boulanger et al. 2014] Single-molecule fluorescence (3-D) Recover pointwise sources from noisy low-resolution observations. Practice: Scalable algorithms? Theory: Rayleigh limit? Perceptron with 1 hidden layer <latexit 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Mixture estimation <latexit 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<latexit 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