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@pierre-haessig
Created July 13, 2015 15:42
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Image plot with a logit scale -- example of a transition matrix
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{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Image plot with logit normalization - example of a transition matrix"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Pierre Haessig -- July 13, 2015"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"**Objective**:\n",
"\n",
"> plot an 2D array (image) with `plt.imshow` using a [logit](https://en.wikipedia.org/wiki/Logit) normalization \n",
"> to **better distinguish** values that are *close to zero* AND values that are *close to one*.\n",
"\n",
"A closely related topic: logit scale\n",
"\n",
"* logit scale for plotting (y-scale), in particular cumulative probabilies: http://nbviewer.ipython.org/gist/pierre-haessig/7e3e6a818edeb6819708\n",
"* Matplotlib Pull Request [#3753](https://github.com/matplotlib/matplotlib/pull/3753) which implements this scale"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"import numpy as np\n",
"import matplotlib.pyplot as plt"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"%matplotlib inline"
]
},
{
"cell_type": "code",
"execution_count": 84,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"from IPython.html.widgets import interact"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Example data"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Example of the transition matrix of a dummy [Markov chain](https://en.wikipedia.org/wiki/Markov_chain#Example) with four states "
]
},
{
"cell_type": "code",
"execution_count": 109,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"text/plain": [
"array([[ 0.9 , 0.05 , 0.04 , 0.01 ],\n",
" [ 0.01 , 0.979, 0.01 , 0.001],\n",
" [ 0. , 0.001, 0.998, 0.001],\n",
" [ 0. , 0.01 , 0.3 , 0.69 ]])"
]
},
"execution_count": 109,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"T = np.array([\n",
" [0.9, 0.05, 0.04, 0.01],\n",
" [0.01, 0.979, 0.01, 0.001],\n",
" [0., 0.001, 0.998, 0.001],\n",
" [0., 0.01, 0.3, 0.69]\n",
" ])\n",
"T"
]
},
{
"cell_type": "code",
"execution_count": 110,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"text/plain": [
"array([ 1., 1., 1., 1.])"
]
},
"execution_count": 110,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"# Property of a transition/stochastic matrix:\n",
"# each row sums to 1\n",
"T.sum(axis=1)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Plotting experiments"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Plot with imshow, choice of colormap"
]
},
{
"cell_type": "code",
"execution_count": 103,
"metadata": {
"collapsed": false
},
"outputs": [],
"source": [
"imopts = dict(interpolation='nearest',\n",
" cmap = 'BuPu_r')\n",
"def plot_T(exponent=1):\n",
" plt.imshow(T**exponent, **imopts)\n",
" plt.xticks(range(4))\n",
" plt.yticks(range(4))\n",
" plt.colorbar()\n",
" if exponent == 1:\n",
" plt.title('linear norm')\n",
" else:\n",
" plt.title('power law with exponent $\\gamma$ = {:}'.format(exponent))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Alternate choice of colormaps"
]
},
{
"cell_type": "code",
"execution_count": 104,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"### Sequential\n",
"#imopts['cmap'] = 'BuPu'\n",
"\n",
"### Diverging\n",
"#imopts['cmap'] = 'RdBu_r'\n",
"#imopts['cmap'] = 'RdYlBu_r'"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### Linear normalization (i.e. no normalization)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Observation:\n",
" \n",
"* Good separation between three groups: values that are close to 1, close to zero, and in between\n",
"* Bad separation at both ends:\n",
" * Values greater than 0.9 are very similar\n",
" * Values smaller than 0.1 are very similar"
]
},
{
"cell_type": "code",
"execution_count": 105,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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0v6K7K8p8+7YI345iNmlFYiMlr+g2y51DycyS0sNLszIcSma580jJzJIyaEsCzGyS80jJ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\nAAAASUVORK5CYII=\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa333d790>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"plot_T()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### \"Square root\" type of linearization"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Better sepation of values close to zero: plot of $T^\\gamma$ with an exponent $\\gamma < 1$\n",
"\n",
"(typically one gets $\\sqrt{T}$ for $\\gamma = 0.5$)\n",
"\n",
"Drawback: compression of the values close to 1"
]
},
{
"cell_type": "code",
"execution_count": 106,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa320c650>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"plot_T(0.3)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### \"Squared\" type of linearization"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"with $\\gamma > 1$, one gets a better separation of values close to one\n",
"\n",
"Drawback: compression of the values close to 0"
]
},
{
"cell_type": "code",
"execution_count": 107,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa2d7a090>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"plot_T(4)"
]
},
{
"cell_type": "code",
"execution_count": 108,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa2cca710>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"interact(plot_T, exponent=[0.2, 5, 0.1]);"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"### Logit normalization"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"the logit transform\n",
"\n",
"$$ a \\mapsto \\log (\\frac{a}{1-a})$$\n",
"\n",
"expands values that are close to zero and close to one"
]
},
{
"cell_type": "code",
"execution_count": 58,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"def logit(a):\n",
" '''logit, with base 10 logarithm'''\n",
" return np.log10(a/(1-a))"
]
},
{
"cell_type": "code",
"execution_count": 80,
"metadata": {
"collapsed": false
},
"outputs": [],
"source": [
"def plot_T_logit(vmax=5):\n",
" # cut values that are zero\n",
" T_sat = np.where(T>0, T, 1e-16)\n",
" lT = logit(T_sat)\n",
" plt.imshow(lT, vmin=-vmax, vmax=vmax, **imopts)\n",
" plt.xticks(range(4))\n",
" plt.yticks(range(4))\n",
" plt.colorbar()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"The logit normalization works best with a diverging colormap"
]
},
{
"cell_type": "code",
"execution_count": 81,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"### Diverging\n",
"imopts['cmap'] = 'RdBu_r'\n",
"#imopts['cmap'] = 'RdYlBu_r'"
]
},
{
"cell_type": "code",
"execution_count": 82,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa33e7290>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"plot_T_logit()"
]
},
{
"cell_type": "code",
"execution_count": 83,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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BrWbX6vOUB7OCGypFrqMRkt4laT0wD7hO0g3Z93tKui4r9spafUdJWpEdC+vV7ZaWWcF1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\nnLTMLCn/D4Yy7RbmL3ysAAAAAElFTkSuQmCC\n",
"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa314c6d0>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"plot_T_logit(3)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Interactive choice of vmax: 4 (which corresponds to minimum probability of 0.0001) seems good for this example"
]
},
{
"cell_type": "code",
"execution_count": 87,
"metadata": {
"collapsed": false
},
"outputs": [
{
"data": {
"image/png": 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"text/plain": [
"<matplotlib.figure.Figure at 0x7f3aa2d820d0>"
]
},
"metadata": {},
"output_type": "display_data"
}
],
"source": [
"interact(plot_T_logit, vmax=[1, 7]);"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 2",
"language": "python",
"name": "python2"
},
"language_info": {
"codemirror_mode": {
"name": "ipython",
"version": 2
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython2",
"version": "2.7.10"
}
},
"nbformat": 4,
"nbformat_minor": 0
}
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