ex-6: improve plots
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from pylab import *
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from pylab import *
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import sys
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import sys
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import matplotlib.pyplot as plt
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plt.rcParams['font.size'] = 20
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rcParams['font.size'] = 12
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a, b, f = loadtxt(sys.stdin, unpack=True)
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a, b, f = loadtxt(sys.stdin, unpack=True)
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suptitle('Fraunhofer diffraction')
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title(sys.argv[1] if len(sys.argv) > 1 else "", loc='right')
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title(sys.argv[1] if len(sys.argv) > 1 else "", loc='right')
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hist(a, np.insert(b, 0, a[0]), weights=f/sum(f),
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hist(a, np.insert(b, 0, a[0]), weights=100*f/sum(f),
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color='#dbbf0d', edgecolor='#595856', linewidth=0.5)
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histtype='stepfilled', color='#e3c5ca', edgecolor='#92182b')
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xlabel(r'$\theta$ (radians)')
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xlabel(r'$\theta$ (radians)')
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ylabel(r'$I(\theta)$ (a.u.)')
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ylabel(r'$I(\theta)$ (a.u.)')
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tight_layout()
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show()
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show()
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notes/images/fraun-conv-0.05.pdf
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notes/images/fraun-conv-0.05.pdf
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notes/images/fraun-conv-0.5.pdf
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notes/images/fraun-conv-0.5.pdf
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notes/images/fraun-conv-1.pdf
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notes/images/fraun-conv-1.pdf
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notes/images/fraun-fft-0.05.pdf
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notes/images/fraun-fft-0.5.pdf
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notes/images/fraun-original.pdf
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notes/images/fraun-original.pdf
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notes/images/fraun-rl-0.05.pdf
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notes/images/fraun-rl-0.5.pdf
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notes/images/fraun-rl-1.pdf
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# Exercise 6
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# Exercise 6
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## Generating points according to Fraunhofer diffraction
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## Generating points according to Fraunhöfer diffraction
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The diffraction of a plane wave thorough a round slit must be simulated by
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The diffraction of a plane wave thorough a round slit must be simulated by
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generating $N =$ 50'000 points according to the intensity distribution
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generating $N =$ 50'000 points according to the intensity distribution
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@ -16,7 +16,7 @@ where:
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- $E$ is the electric field amplitude, default set $E = \SI{1e4}{V/m}$;
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- $E$ is the electric field amplitude, default set $E = \SI{1e4}{V/m}$;
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- $a$ is the radius of the slit aperture, default set $a = \SI{0.01}{m}$;
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- $a$ is the radius of the slit aperture, default set $a = \SI{0.01}{m}$;
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- $\theta$ is the angle specified in @fig:slit;
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- $\theta$ is the angle specified in @fig:slit;
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- $J_1$ is the Bessel function of first order;
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- $J_1$ is a Bessel function of first kind;
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- $k$ is the wavenumber, default set $k = \SI{1e-4}{m^{-1}}$;
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- $k$ is the wavenumber, default set $k = \SI{1e-4}{m^{-1}}$;
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- $L$ default set $L = \SI{1}{m}$.
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- $L$ default set $L = \SI{1}{m}$.
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@ -46,7 +46,7 @@ where:
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\node [cyclamen] at (5.5,-0.4) {$\theta$};
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\node [cyclamen] at (5.5,-0.4) {$\theta$};
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\node [rotate=-90] at (10.2,0) {screen};
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\node [rotate=-90] at (10.2,0) {screen};
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\end{tikzpicture}
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\end{tikzpicture}
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\caption{Fraunhofer diffraction.}\label{fig:slit}
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\caption{Fraunhöfer diffraction.}\label{fig:slit}
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}
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}
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\end{figure}
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\end{figure}
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@ -88,8 +88,7 @@ omitted:
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The sample was binned and stored in a histogram with a customizable number $n$
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The sample was binned and stored in a histogram with a customizable number $n$
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of bins default set $n = 150$. In @fig:original an example is shown.
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of bins default set $n = 150$. In @fig:original an example is shown.
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![Example of sorted points according to
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![Example of an intensity histogram.](images/fraun-original.pdf){#fig:original}
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$I(\theta)$.](images/6_original.pdf){#fig:original}
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## Gaussian noise convolution {#sec:convolution}
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## Gaussian noise convolution {#sec:convolution}
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@ -417,41 +416,41 @@ On the other hand, the Richardson-Lucy routine is less affected by this further
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complication being already inaccurate in itself.
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complication being already inaccurate in itself.
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<div id="fig:results1">
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<div id="fig:results1">
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![Convolved signal.](images/noise-0.05.pdf){width=12cm}
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![Convolved signal.](images/fraun-conv-0.05.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/deco-fft-0.05.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/fraun-fft-0.05.pdf){width=12cm}
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![Deconvolved signal with RL.](images/deco-rl-0.05.pdf){width=12cm}
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![Deconvolved signal with RL.](images/fraun-rl-0.05.pdf){width=12cm}
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Results for $\sigma = 0.05 \Delta \theta$, where $\Delta \theta$ is the bin
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Results for $\sigma = 0.05 \Delta \theta$, where $\Delta \theta$ is the bin
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width.
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width.
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</div>
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</div>
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<div id="fig:results2">
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<div id="fig:results2">
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![Convolved signal.](images/noise-0.5.pdf){width=12cm}
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![Convolved signal.](images/fraun-conv-0.5.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/deco-fft-0.5.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/fraun-fft-0.5.pdf){width=12cm}
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![Deconvolved signal with RL.](images/deco-rl-0.5.pdf){width=12cm}
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![Deconvolved signal with RL.](images/fraun-rl-0.5.pdf){width=12cm}
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Results for $\sigma = 0.5 \Delta \theta$, where $\Delta \theta$ is the bin
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Results for $\sigma = 0.5 \Delta \theta$, where $\Delta \theta$ is the bin
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width.
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width.
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</div>
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</div>
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<div id="fig:results3">
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<div id="fig:results3">
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![Convolved signal.](images/noise-1.pdf){width=12cm}
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![Convolved signal.](images/fraun-conv-1.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/deco-fft-1.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/fraun-fft-1.pdf){width=12cm}
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![Deconvolved signal with RL.](images/deco-rl-1.pdf){width=12cm}
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![Deconvolved signal with RL.](images/fraun-rl-1.pdf){width=12cm}
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Results for $\sigma = \Delta \theta$, where $\Delta \theta$ is the bin width.
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Results for $\sigma = \Delta \theta$, where $\Delta \theta$ is the bin width.
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</div>
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</div>
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<div id="fig:poisson">
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<div id="fig:poisson">
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![Deconvolved signal with FFT.](images/poisson-fft.pdf){width=12cm}
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![Deconvolved signal with FFT.](images/fraun-noise-fft.pdf){width=12cm}
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![Deconvolved signal withh RL.](images/poisson-rl.pdf){width=12cm}
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![Deconvolved signal withh RL.](images/fraun-noise-rl.pdf){width=12cm}
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Results for $\sigma = \Delta \theta$, poissoned data.
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Results for $\sigma = \Delta \theta$, with Poisson noise.
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</div>
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</div>
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