1 | ##################################################################### |
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2 | #This software was developed by the University of Tennessee as part of the |
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3 | #Distributed Data Analysis of Neutron Scattering Experiments (DANSE) |
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4 | #project funded by the US National Science Foundation. |
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5 | #See the license text in license.txt |
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6 | #copyright 2010, University of Tennessee |
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7 | ###################################################################### |
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8 | |
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9 | """ |
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10 | This module implements invariant and its related computations. |
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11 | |
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12 | :author: Gervaise B. Alina/UTK |
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13 | :author: Mathieu Doucet/UTK |
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14 | :author: Jae Cho/UTK |
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15 | |
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16 | """ |
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17 | import math |
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18 | import numpy |
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19 | |
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20 | from sans.dataloader.data_info import Data1D as LoaderData1D |
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21 | |
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22 | # The minimum q-value to be used when extrapolating |
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23 | Q_MINIMUM = 1e-5 |
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24 | |
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25 | # The maximum q-value to be used when extrapolating |
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26 | Q_MAXIMUM = 10 |
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27 | |
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28 | # Number of steps in the extrapolation |
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29 | INTEGRATION_NSTEPS = 1000 |
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30 | |
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31 | class Transform(object): |
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32 | """ |
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33 | Define interface that need to compute a function or an inverse |
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34 | function given some x, y |
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35 | """ |
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36 | |
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37 | def linearize_data(self, data): |
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38 | """ |
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39 | Linearize data so that a linear fit can be performed. |
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40 | Filter out the data that can't be transformed. |
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41 | |
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42 | :param data: LoadData1D instance |
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43 | |
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44 | """ |
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45 | # Check that the vector lengths are equal |
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46 | assert(len(data.x)==len(data.y)) |
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47 | if data.dy is not None: |
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48 | assert(len(data.x)==len(data.dy)) |
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49 | dy = data.dy |
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50 | else: |
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51 | dy = numpy.ones(len(data.y)) |
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52 | |
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53 | # Transform the data |
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54 | data_points = zip(data.x, data.y, dy) |
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55 | |
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56 | output_points = [(self.linearize_q_value(p[0]), |
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57 | math.log(p[1]), |
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58 | p[2]/p[1]) for p in data_points if p[0]>0 and \ |
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59 | p[1]>0 and p[2]>0] |
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60 | |
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61 | x_out, y_out, dy_out = zip(*output_points) |
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62 | |
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63 | # Create Data1D object |
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64 | x_out = numpy.asarray(x_out) |
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65 | y_out = numpy.asarray(y_out) |
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66 | dy_out = numpy.asarray(dy_out) |
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67 | linear_data = LoaderData1D(x=x_out, y=y_out, dy=dy_out) |
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68 | |
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69 | return linear_data |
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70 | |
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71 | def get_allowed_bins(self, data): |
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72 | """ |
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73 | Goes through the data points and returns a list of boolean values |
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74 | to indicate whether each points is allowed by the model or not. |
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75 | |
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76 | :param data: Data1D object |
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77 | """ |
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78 | return [p[0]>0 and p[1]>0 and p[2]>0 for p in zip(data.x, data.y, |
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79 | data.dy)] |
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80 | |
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81 | def linearize_q_value(self, value): |
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82 | """ |
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83 | Transform the input q-value for linearization |
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84 | """ |
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85 | return NotImplemented |
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86 | |
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87 | def extract_model_parameters(self, constant, slope, dconstant=0, dslope=0): |
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88 | """ |
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89 | set private member |
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90 | """ |
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91 | return NotImplemented |
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92 | |
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93 | def evaluate_model(self, x): |
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94 | """ |
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95 | Returns an array f(x) values where f is the Transform function. |
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96 | """ |
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97 | return NotImplemented |
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98 | |
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99 | def evaluate_model_errors(self, x): |
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100 | """ |
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101 | Returns an array of I(q) errors |
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102 | """ |
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103 | return NotImplemented |
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104 | |
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105 | class Guinier(Transform): |
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106 | """ |
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107 | class of type Transform that performs operations related to guinier |
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108 | function |
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109 | """ |
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110 | def __init__(self, scale=1, radius=60): |
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111 | Transform.__init__(self) |
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112 | self.scale = scale |
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113 | self.radius = radius |
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114 | ## Uncertainty of scale parameter |
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115 | self.dscale = 0 |
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116 | ## Unvertainty of radius parameter |
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117 | self.dradius = 0 |
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118 | |
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119 | def linearize_q_value(self, value): |
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120 | """ |
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121 | Transform the input q-value for linearization |
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122 | |
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123 | :param value: q-value |
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124 | |
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125 | :return: q*q |
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126 | """ |
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127 | return value * value |
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128 | |
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129 | def extract_model_parameters(self, constant, slope, dconstant=0, dslope=0): |
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130 | """ |
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131 | assign new value to the scale and the radius |
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132 | """ |
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133 | self.scale = math.exp(constant) |
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134 | self.radius = math.sqrt(-3 * slope) |
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135 | |
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136 | # Errors |
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137 | self.dscale = math.exp(constant)*dconstant |
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138 | self.dradius = -3.0/2.0/math.sqrt(-3 * slope)*dslope |
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139 | |
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140 | return [self.radius, self.scale], [self.dradius, self.dscale] |
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141 | |
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142 | def evaluate_model(self, x): |
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143 | """ |
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144 | return F(x)= scale* e-((radius*x)**2/3) |
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145 | """ |
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146 | return self._guinier(x) |
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147 | |
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148 | def evaluate_model_errors(self, x): |
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149 | """ |
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150 | Returns the error on I(q) for the given array of q-values |
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151 | |
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152 | :param x: array of q-values |
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153 | """ |
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154 | p1 = numpy.array([self.dscale * math.exp(-((self.radius * q)**2/3)) \ |
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155 | for q in x]) |
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156 | p2 = numpy.array([self.scale * math.exp(-((self.radius * q)**2/3))\ |
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157 | * (-(q**2/3)) * 2 * self.radius * self.dradius for q in x]) |
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158 | diq2 = p1*p1 + p2*p2 |
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159 | return numpy.array( [math.sqrt(err) for err in diq2] ) |
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160 | |
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161 | def _guinier(self, x): |
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162 | """ |
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163 | Retrive the guinier function after apply an inverse guinier function |
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164 | to x |
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165 | Compute a F(x) = scale* e-((radius*x)**2/3). |
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166 | |
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167 | :param x: a vector of q values |
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168 | :param scale: the scale value |
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169 | :param radius: the guinier radius value |
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170 | |
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171 | :return: F(x) |
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172 | """ |
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173 | # transform the radius of coming from the inverse guinier function to a |
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174 | # a radius of a guinier function |
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175 | if self.radius <= 0: |
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176 | msg = "Rg expected positive value, but got %s"%self.radius |
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177 | raise ValueError(msg) |
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178 | value = numpy.array([math.exp(-((self.radius * i)**2/3)) for i in x ]) |
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179 | return self.scale * value |
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180 | |
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181 | class PowerLaw(Transform): |
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182 | """ |
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183 | class of type transform that perform operation related to power_law |
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184 | function |
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185 | """ |
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186 | def __init__(self, scale=1, power=4): |
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187 | Transform.__init__(self) |
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188 | self.scale = scale |
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189 | self.power = power |
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190 | |
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191 | def linearize_q_value(self, value): |
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192 | """ |
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193 | Transform the input q-value for linearization |
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194 | |
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195 | :param value: q-value |
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196 | |
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197 | :return: log(q) |
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198 | """ |
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199 | return math.log(value) |
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200 | |
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201 | def extract_model_parameters(self, constant, slope, dconstant=0, dslope=0): |
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202 | """ |
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203 | Assign new value to the scale and the power |
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204 | """ |
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205 | self.power = -slope |
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206 | self.scale = math.exp(constant) |
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207 | |
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208 | # Errors |
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209 | self.dscale = math.exp(constant)*dconstant |
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210 | self.dpower = -dslope |
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211 | |
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212 | return [self.power, self.scale], [self.dpower, self.dscale] |
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213 | |
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214 | def evaluate_model(self, x): |
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215 | """ |
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216 | given a scale and a radius transform x, y using a power_law |
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217 | function |
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218 | """ |
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219 | return self._power_law(x) |
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220 | |
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221 | def evaluate_model_errors(self, x): |
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222 | """ |
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223 | Returns the error on I(q) for the given array of q-values |
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224 | :param x: array of q-values |
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225 | """ |
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226 | p1 = numpy.array([self.dscale * math.pow(q, -self.power) for q in x]) |
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227 | p2 = numpy.array([self.scale * self.power * math.pow(q, -self.power-1)\ |
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228 | * self.dpower for q in x]) |
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229 | diq2 = p1*p1 + p2*p2 |
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230 | return numpy.array( [math.sqrt(err) for err in diq2] ) |
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231 | |
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232 | def _power_law(self, x): |
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233 | """ |
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234 | F(x) = scale* (x)^(-power) |
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235 | when power= 4. the model is porod |
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236 | else power_law |
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237 | The model has three parameters: :: |
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238 | 1. x: a vector of q values |
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239 | 2. power: power of the function |
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240 | 3. scale : scale factor value |
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241 | |
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242 | :param x: array |
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243 | :return: F(x) |
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244 | """ |
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245 | if self.power <= 0: |
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246 | msg = "Power_law function expected positive power," |
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247 | msg += " but got %s"%self.power |
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248 | raise ValueError(msg) |
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249 | if self.scale <= 0: |
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250 | msg = "scale expected positive value, but got %s"%self.scale |
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251 | raise ValueError(msg) |
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252 | |
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253 | value = numpy.array([ math.pow(i, -self.power) for i in x ]) |
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254 | return self.scale * value |
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255 | |
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256 | class Extrapolator: |
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257 | """ |
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258 | Extrapolate I(q) distribution using a given model |
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259 | """ |
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260 | def __init__(self, data, model=None): |
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261 | """ |
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262 | Determine a and b given a linear equation y = ax + b |
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263 | |
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264 | If a model is given, it will be used to linearize the data before |
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265 | the extrapolation is performed. If None, |
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266 | a simple linear fit will be done. |
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267 | |
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268 | :param data: data containing x and y such as y = ax + b |
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269 | :param model: optional Transform object |
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270 | """ |
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271 | self.data = data |
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272 | self.model = model |
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273 | |
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274 | # Set qmin as the lowest non-zero value |
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275 | self.qmin = Q_MINIMUM |
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276 | for q_value in self.data.x: |
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277 | if q_value > 0: |
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278 | self.qmin = q_value |
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279 | break |
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280 | self.qmax = max(self.data.x) |
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281 | |
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282 | def fit(self, power=None, qmin=None, qmax=None): |
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283 | """ |
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284 | Fit data for y = ax + b return a and b |
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285 | |
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286 | :param power: a fixed, otherwise None |
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287 | :param qmin: Minimum Q-value |
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288 | :param qmax: Maximum Q-value |
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289 | """ |
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290 | if qmin is None: |
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291 | qmin = self.qmin |
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292 | if qmax is None: |
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293 | qmax = self.qmax |
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294 | |
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295 | # Identify the bin range for the fit |
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296 | idx = (self.data.x >= qmin) & (self.data.x <= qmax) |
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297 | |
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298 | fx = numpy.zeros(len(self.data.x)) |
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299 | |
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300 | # Uncertainty |
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301 | if type(self.data.dy)==numpy.ndarray and \ |
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302 | len(self.data.dy)==len(self.data.x) and \ |
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303 | numpy.all(self.data.dy>0): |
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304 | sigma = self.data.dy |
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305 | else: |
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306 | sigma = numpy.ones(len(self.data.x)) |
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307 | |
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308 | # Compute theory data f(x) |
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309 | fx[idx] = self.data.y[idx] |
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310 | |
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311 | # Linearize the data |
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312 | if self.model is not None: |
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313 | linearized_data = self.model.linearize_data(\ |
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314 | LoaderData1D(self.data.x[idx], |
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315 | fx[idx], |
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316 | dy = sigma[idx])) |
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317 | else: |
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318 | linearized_data = LoaderData1D(self.data.x[idx], |
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319 | fx[idx], |
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320 | dy = sigma[idx]) |
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321 | |
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322 | ##power is given only for function = power_law |
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323 | if power != None: |
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324 | sigma2 = linearized_data.dy * linearized_data.dy |
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325 | a = -(power) |
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326 | b = (numpy.sum(linearized_data.y/sigma2) \ |
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327 | - a*numpy.sum(linearized_data.x/sigma2))/numpy.sum(1.0/sigma2) |
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328 | |
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329 | |
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330 | deltas = linearized_data.x*a + \ |
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331 | numpy.ones(len(linearized_data.x))*b-linearized_data.y |
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332 | residuals = numpy.sum(deltas*deltas/sigma2) |
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333 | |
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334 | err = math.fabs(residuals) / numpy.sum(1.0/sigma2) |
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335 | return [a, b], [0, math.sqrt(err)] |
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336 | else: |
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337 | A = numpy.vstack([ linearized_data.x/linearized_data.dy, |
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338 | 1.0/linearized_data.dy]).T |
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339 | (p, residuals, rank, s) = numpy.linalg.lstsq(A, |
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340 | linearized_data.y/linearized_data.dy) |
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341 | |
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342 | # Get the covariance matrix, defined as inv_cov = a_transposed * a |
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343 | err = numpy.zeros(2) |
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344 | try: |
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345 | inv_cov = numpy.dot(A.transpose(), A) |
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346 | cov = numpy.linalg.pinv(inv_cov) |
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347 | err_matrix = math.fabs(residuals) * cov |
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348 | err = [math.sqrt(err_matrix[0][0]), math.sqrt(err_matrix[1][1])] |
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349 | except: |
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350 | err = [-1.0, -1.0] |
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351 | |
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352 | return p, err |
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353 | |
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354 | |
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355 | class InvariantCalculator(object): |
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356 | """ |
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357 | Compute invariant if data is given. |
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358 | Can provide volume fraction and surface area if the user provides |
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359 | Porod constant and contrast values. |
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360 | |
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361 | :precondition: the user must send a data of type DataLoader.Data1D |
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362 | the user provide background and scale values. |
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363 | |
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364 | :note: Some computations depends on each others. |
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365 | """ |
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366 | def __init__(self, data, background=0, scale=1 ): |
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367 | """ |
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368 | Initialize variables. |
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369 | |
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370 | :param data: data must be of type DataLoader.Data1D |
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371 | :param background: Background value. The data will be corrected |
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372 | before processing |
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373 | :param scale: Scaling factor for I(q). The data will be corrected |
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374 | before processing |
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375 | """ |
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376 | # Background and scale should be private data member if the only way to |
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377 | # change them are by instantiating a new object. |
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378 | self._background = background |
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379 | self._scale = scale |
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380 | # slit height for smeared data |
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381 | self._smeared = None |
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382 | # The data should be private |
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383 | self._data = self._get_data(data) |
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384 | # get the dxl if the data is smeared: This is done only once on init. |
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385 | if self._data.dxl != None and self._data.dxl.all() >0: |
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386 | # assumes constant dxl |
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387 | self._smeared = self._data.dxl[0] |
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388 | |
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389 | # Since there are multiple variants of Q*, you should force the |
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390 | # user to use the get method and keep Q* a private data member |
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391 | self._qstar = None |
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392 | |
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393 | # You should keep the error on Q* so you can reuse it without |
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394 | # recomputing the whole thing. |
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395 | self._qstar_err = 0 |
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396 | |
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397 | # Extrapolation parameters |
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398 | self._low_extrapolation_npts = 4 |
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399 | self._low_extrapolation_function = Guinier() |
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400 | self._low_extrapolation_power = None |
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401 | self._low_extrapolation_power_fitted = None |
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402 | |
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403 | self._high_extrapolation_npts = 4 |
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404 | self._high_extrapolation_function = PowerLaw() |
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405 | self._high_extrapolation_power = None |
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406 | self._high_extrapolation_power_fitted = None |
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407 | |
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408 | # Extrapolation range |
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409 | self._low_q_limit = Q_MINIMUM |
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410 | |
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411 | def _get_data(self, data): |
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412 | """ |
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413 | :note: this function must be call before computing any type |
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414 | of invariant |
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415 | |
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416 | :return: new data = self._scale *data - self._background |
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417 | """ |
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418 | if not issubclass(data.__class__, LoaderData1D): |
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419 | #Process only data that inherited from DataLoader.Data_info.Data1D |
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420 | raise ValueError,"Data must be of type DataLoader.Data1D" |
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421 | #from copy import deepcopy |
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422 | new_data = (self._scale * data) - self._background |
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423 | |
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424 | # Check that the vector lengths are equal |
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425 | assert(len(new_data.x)==len(new_data.y)) |
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426 | |
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427 | # Verify that the errors are set correctly |
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428 | if new_data.dy is None or len(new_data.x) != len(new_data.dy) or \ |
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429 | (min(new_data.dy)==0 and max(new_data.dy)==0): |
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430 | new_data.dy = numpy.ones(len(new_data.x)) |
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431 | return new_data |
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432 | |
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433 | def _fit(self, model, qmin=Q_MINIMUM, qmax=Q_MAXIMUM, power=None): |
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434 | """ |
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435 | fit data with function using |
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436 | data = self._get_data() |
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437 | fx = Functor(data , function) |
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438 | y = data.y |
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439 | slope, constant = linalg.lstsq(y,fx) |
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440 | |
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441 | :param qmin: data first q value to consider during the fit |
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442 | :param qmax: data last q value to consider during the fit |
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443 | :param power : power value to consider for power-law |
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444 | :param function: the function to use during the fit |
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445 | |
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446 | :return a: the scale of the function |
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447 | :return b: the other parameter of the function for guinier will be radius |
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448 | for power_law will be the power value |
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449 | """ |
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450 | extrapolator = Extrapolator(data=self._data, model=model) |
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451 | p, dp = extrapolator.fit(power=power, qmin=qmin, qmax=qmax) |
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452 | |
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453 | return model.extract_model_parameters(constant=p[1], slope=p[0], |
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454 | dconstant=dp[1], dslope=dp[0]) |
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455 | |
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456 | def _get_qstar(self, data): |
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457 | """ |
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458 | Compute invariant for pinhole data. |
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459 | This invariant is given by: :: |
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460 | |
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461 | q_star = x0**2 *y0 *dx0 +x1**2 *y1 *dx1 |
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462 | + ..+ xn**2 *yn *dxn for non smeared data |
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463 | |
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464 | q_star = dxl0 *x0 *y0 *dx0 +dxl1 *x1 *y1 *dx1 |
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465 | + ..+ dlxn *xn *yn *dxn for smeared data |
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466 | |
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467 | where n >= len(data.x)-1 |
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468 | dxl = slit height dQl |
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469 | dxi = 1/2*(xi+1 - xi) + (xi - xi-1) |
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470 | dx0 = (x1 - x0)/2 |
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471 | dxn = (xn - xn-1)/2 |
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472 | |
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473 | :param data: the data to use to compute invariant. |
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474 | |
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475 | :return q_star: invariant value for pinhole data. q_star > 0 |
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476 | """ |
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477 | if len(data.x) <= 1 or len(data.y) <= 1 or len(data.x)!= len(data.y): |
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478 | msg = "Length x and y must be equal" |
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479 | msg += " and greater than 1; got x=%s, y=%s"%(len(data.x), |
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480 | len(data.y)) |
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481 | raise ValueError, msg |
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482 | else: |
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483 | # Take care of smeared data |
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484 | if self._smeared is None: |
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485 | gx = data.x * data.x |
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486 | # assumes that len(x) == len(dxl). |
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487 | else: |
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488 | gx = data.dxl * data.x |
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489 | |
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490 | n = len(data.x)- 1 |
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491 | #compute the first delta q |
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492 | dx0 = (data.x[1] - data.x[0])/2 |
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493 | #compute the last delta q |
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494 | dxn = (data.x[n] - data.x[n-1])/2 |
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495 | sum = 0 |
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496 | sum += gx[0] * data.y[0] * dx0 |
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497 | sum += gx[n] * data.y[n] * dxn |
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498 | |
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499 | if len(data.x) == 2: |
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500 | return sum |
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501 | else: |
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502 | #iterate between for element different |
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503 | #from the first and the last |
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504 | for i in xrange(1, n-1): |
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505 | dxi = (data.x[i+1] - data.x[i-1])/2 |
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506 | sum += gx[i] * data.y[i] * dxi |
---|
507 | return sum |
---|
508 | |
---|
509 | def _get_qstar_uncertainty(self, data): |
---|
510 | """ |
---|
511 | Compute invariant uncertainty with with pinhole data. |
---|
512 | This uncertainty is given as follow: :: |
---|
513 | |
---|
514 | dq_star = math.sqrt[(x0**2*(dy0)*dx0)**2 + |
---|
515 | (x1**2 *(dy1)*dx1)**2 + ..+ (xn**2 *(dyn)*dxn)**2 ] |
---|
516 | where n >= len(data.x)-1 |
---|
517 | dxi = 1/2*(xi+1 - xi) + (xi - xi-1) |
---|
518 | dx0 = (x1 - x0)/2 |
---|
519 | dxn = (xn - xn-1)/2 |
---|
520 | dyn: error on dy |
---|
521 | |
---|
522 | :param data: |
---|
523 | :note: if data doesn't contain dy assume dy= math.sqrt(data.y) |
---|
524 | """ |
---|
525 | if len(data.x) <= 1 or len(data.y) <= 1 or \ |
---|
526 | len(data.x) != len(data.y) or \ |
---|
527 | (data.dy is not None and (len(data.dy) != len(data.y))): |
---|
528 | msg = "Length of data.x and data.y must be equal" |
---|
529 | msg += " and greater than 1; got x=%s, y=%s"%(len(data.x), |
---|
530 | len(data.y)) |
---|
531 | raise ValueError, msg |
---|
532 | else: |
---|
533 | #Create error for data without dy error |
---|
534 | if data.dy is None: |
---|
535 | dy = math.sqrt(data.y) |
---|
536 | else: |
---|
537 | dy = data.dy |
---|
538 | # Take care of smeared data |
---|
539 | if self._smeared is None: |
---|
540 | gx = data.x * data.x |
---|
541 | # assumes that len(x) == len(dxl). |
---|
542 | else: |
---|
543 | gx = data.dxl * data.x |
---|
544 | |
---|
545 | n = len(data.x) - 1 |
---|
546 | #compute the first delta |
---|
547 | dx0 = (data.x[1] - data.x[0])/2 |
---|
548 | #compute the last delta |
---|
549 | dxn= (data.x[n] - data.x[n-1])/2 |
---|
550 | sum = 0 |
---|
551 | sum += (gx[0] * dy[0] * dx0)**2 |
---|
552 | sum += (gx[n] * dy[n] * dxn)**2 |
---|
553 | if len(data.x) == 2: |
---|
554 | return math.sqrt(sum) |
---|
555 | else: |
---|
556 | #iterate between for element different |
---|
557 | #from the first and the last |
---|
558 | for i in xrange(1, n-1): |
---|
559 | dxi = (data.x[i+1] - data.x[i-1])/2 |
---|
560 | sum += (gx[i] * dy[i] * dxi)**2 |
---|
561 | return math.sqrt(sum) |
---|
562 | |
---|
563 | def _get_extrapolated_data(self, model, npts=INTEGRATION_NSTEPS, |
---|
564 | q_start=Q_MINIMUM, q_end=Q_MAXIMUM): |
---|
565 | """ |
---|
566 | :return: extrapolate data create from data |
---|
567 | """ |
---|
568 | #create new Data1D to compute the invariant |
---|
569 | q = numpy.linspace(start=q_start, |
---|
570 | stop=q_end, |
---|
571 | num=npts, |
---|
572 | endpoint=True) |
---|
573 | iq = model.evaluate_model(q) |
---|
574 | diq = model.evaluate_model_errors(q) |
---|
575 | |
---|
576 | result_data = LoaderData1D(x=q, y=iq, dy=diq) |
---|
577 | if self._smeared != None: |
---|
578 | result_data.dxl = self._smeared * numpy.ones(len(q)) |
---|
579 | return result_data |
---|
580 | |
---|
581 | def get_data(self): |
---|
582 | """ |
---|
583 | :return: self._data |
---|
584 | """ |
---|
585 | return self._data |
---|
586 | |
---|
587 | def get_extrapolation_power(self, range='high'): |
---|
588 | """ |
---|
589 | :return: the fitted power for power law function for a given |
---|
590 | extrapolation range |
---|
591 | """ |
---|
592 | if range == 'low': |
---|
593 | return self._low_extrapolation_power_fitted |
---|
594 | return self._high_extrapolation_power_fitted |
---|
595 | |
---|
596 | def get_qstar_low(self): |
---|
597 | """ |
---|
598 | Compute the invariant for extrapolated data at low q range. |
---|
599 | |
---|
600 | Implementation: |
---|
601 | data = self._get_extra_data_low() |
---|
602 | return self._get_qstar() |
---|
603 | |
---|
604 | :return q_star: the invariant for data extrapolated at low q. |
---|
605 | """ |
---|
606 | # Data boundaries for fitting |
---|
607 | qmin = self._data.x[0] |
---|
608 | qmax = self._data.x[self._low_extrapolation_npts - 1] |
---|
609 | |
---|
610 | # Extrapolate the low-Q data |
---|
611 | p, dp = self._fit(model=self._low_extrapolation_function, |
---|
612 | qmin=qmin, |
---|
613 | qmax=qmax, |
---|
614 | power=self._low_extrapolation_power) |
---|
615 | self._low_extrapolation_power_fitted = p[0] |
---|
616 | |
---|
617 | # Distribution starting point |
---|
618 | self._low_q_limit = Q_MINIMUM |
---|
619 | if Q_MINIMUM >= qmin: |
---|
620 | self._low_q_limit = qmin/10 |
---|
621 | |
---|
622 | data = self._get_extrapolated_data(\ |
---|
623 | model=self._low_extrapolation_function, |
---|
624 | npts=INTEGRATION_NSTEPS, |
---|
625 | q_start=self._low_q_limit, q_end=qmin) |
---|
626 | |
---|
627 | # Systematic error |
---|
628 | # If we have smearing, the shape of the I(q) distribution at low Q will |
---|
629 | # may not be a Guinier or simple power law. The following is |
---|
630 | # a conservative estimation for the systematic error. |
---|
631 | err = qmin*qmin*math.fabs((qmin-self._low_q_limit)*\ |
---|
632 | (data.y[0] - data.y[INTEGRATION_NSTEPS-1])) |
---|
633 | return self._get_qstar(data), self._get_qstar_uncertainty(data)+err |
---|
634 | |
---|
635 | def get_qstar_high(self): |
---|
636 | """ |
---|
637 | Compute the invariant for extrapolated data at high q range. |
---|
638 | |
---|
639 | Implementation: |
---|
640 | data = self._get_extra_data_high() |
---|
641 | return self._get_qstar() |
---|
642 | |
---|
643 | :return q_star: the invariant for data extrapolated at high q. |
---|
644 | """ |
---|
645 | # Data boundaries for fitting |
---|
646 | x_len = len(self._data.x) - 1 |
---|
647 | qmin = self._data.x[x_len - (self._high_extrapolation_npts - 1)] |
---|
648 | qmax = self._data.x[x_len] |
---|
649 | |
---|
650 | # fit the data with a model to get the appropriate parameters |
---|
651 | p, dp = self._fit(model=self._high_extrapolation_function, |
---|
652 | qmin=qmin, |
---|
653 | qmax=qmax, |
---|
654 | power=self._high_extrapolation_power) |
---|
655 | self._high_extrapolation_power_fitted = p[0] |
---|
656 | |
---|
657 | #create new Data1D to compute the invariant |
---|
658 | data = self._get_extrapolated_data(\ |
---|
659 | model=self._high_extrapolation_function, |
---|
660 | npts=INTEGRATION_NSTEPS, |
---|
661 | q_start=qmax, q_end=Q_MAXIMUM) |
---|
662 | |
---|
663 | return self._get_qstar(data), self._get_qstar_uncertainty(data) |
---|
664 | |
---|
665 | def get_extra_data_low(self, npts_in=None, q_start=None, npts=20): |
---|
666 | """ |
---|
667 | Returns the extrapolated data used for the loew-Q invariant calculation. |
---|
668 | By default, the distribution will cover the data points used for the |
---|
669 | extrapolation. The number of overlap points is a parameter (npts_in). |
---|
670 | By default, the maximum q-value of the distribution will be |
---|
671 | the minimum q-value used when extrapolating for the purpose of the |
---|
672 | invariant calculation. |
---|
673 | |
---|
674 | :param npts_in: number of data points for which |
---|
675 | the extrapolated data overlap |
---|
676 | :param q_start: is the minimum value to uses for extrapolated data |
---|
677 | :param npts: the number of points in the extrapolated distribution |
---|
678 | |
---|
679 | """ |
---|
680 | # Get extrapolation range |
---|
681 | if q_start is None: |
---|
682 | q_start = self._low_q_limit |
---|
683 | |
---|
684 | if npts_in is None: |
---|
685 | npts_in = self._low_extrapolation_npts |
---|
686 | q_end = self._data.x[max(0, npts_in-1)] |
---|
687 | |
---|
688 | if q_start >= q_end: |
---|
689 | return numpy.zeros(0), numpy.zeros(0) |
---|
690 | |
---|
691 | return self._get_extrapolated_data(\ |
---|
692 | model=self._low_extrapolation_function, |
---|
693 | npts=npts, |
---|
694 | q_start=q_start, q_end=q_end) |
---|
695 | |
---|
696 | def get_extra_data_high(self, npts_in=None, q_end=Q_MAXIMUM, npts=20): |
---|
697 | """ |
---|
698 | Returns the extrapolated data used for the high-Q invariant calculation. |
---|
699 | By default, the distribution will cover the data points used for the |
---|
700 | extrapolation. The number of overlap points is a parameter (npts_in). |
---|
701 | By default, the maximum q-value of the distribution will be Q_MAXIMUM, |
---|
702 | the maximum q-value used when extrapolating for the purpose of the |
---|
703 | invariant calculation. |
---|
704 | |
---|
705 | :param npts_in: number of data points for which the |
---|
706 | extrapolated data overlap |
---|
707 | :param q_end: is the maximum value to uses for extrapolated data |
---|
708 | :param npts: the number of points in the extrapolated distribution |
---|
709 | """ |
---|
710 | # Get extrapolation range |
---|
711 | if npts_in is None: |
---|
712 | npts_in = self._high_extrapolation_npts |
---|
713 | _npts = len(self._data.x) |
---|
714 | q_start = self._data.x[min(_npts, _npts-npts_in)] |
---|
715 | |
---|
716 | if q_start >= q_end: |
---|
717 | return numpy.zeros(0), numpy.zeros(0) |
---|
718 | |
---|
719 | return self._get_extrapolated_data(\ |
---|
720 | model=self._high_extrapolation_function, |
---|
721 | npts=npts, |
---|
722 | q_start=q_start, q_end=q_end) |
---|
723 | |
---|
724 | def set_extrapolation(self, range, npts=4, function=None, power=None): |
---|
725 | """ |
---|
726 | Set the extrapolation parameters for the high or low Q-range. |
---|
727 | Note that this does not turn extrapolation on or off. |
---|
728 | |
---|
729 | :param range: a keyword set the type of extrapolation . type string |
---|
730 | :param npts: the numbers of q points of data to consider |
---|
731 | for extrapolation |
---|
732 | :param function: a keyword to select the function to use |
---|
733 | for extrapolation. |
---|
734 | of type string. |
---|
735 | :param power: an power to apply power_low function |
---|
736 | |
---|
737 | """ |
---|
738 | range = range.lower() |
---|
739 | if range not in ['high', 'low']: |
---|
740 | raise ValueError, "Extrapolation range should be 'high' or 'low'" |
---|
741 | function = function.lower() |
---|
742 | if function not in ['power_law', 'guinier']: |
---|
743 | msg = "Extrapolation function should be 'guinier' or 'power_law'" |
---|
744 | raise ValueError, msg |
---|
745 | |
---|
746 | if range == 'high': |
---|
747 | if function != 'power_law': |
---|
748 | msg = "Extrapolation only allows a power law at high Q" |
---|
749 | raise ValueError, msg |
---|
750 | self._high_extrapolation_npts = npts |
---|
751 | self._high_extrapolation_power = power |
---|
752 | self._high_extrapolation_power_fitted = power |
---|
753 | else: |
---|
754 | if function == 'power_law': |
---|
755 | self._low_extrapolation_function = PowerLaw() |
---|
756 | else: |
---|
757 | self._low_extrapolation_function = Guinier() |
---|
758 | self._low_extrapolation_npts = npts |
---|
759 | self._low_extrapolation_power = power |
---|
760 | self._low_extrapolation_power_fitted = power |
---|
761 | |
---|
762 | def get_qstar(self, extrapolation=None): |
---|
763 | """ |
---|
764 | Compute the invariant of the local copy of data. |
---|
765 | |
---|
766 | :param extrapolation: string to apply optional extrapolation |
---|
767 | |
---|
768 | :return q_star: invariant of the data within data's q range |
---|
769 | |
---|
770 | :warning: When using setting data to Data1D , |
---|
771 | the user is responsible of |
---|
772 | checking that the scale and the background are |
---|
773 | properly apply to the data |
---|
774 | |
---|
775 | """ |
---|
776 | self._qstar = self._get_qstar(self._data) |
---|
777 | self._qstar_err = self._get_qstar_uncertainty(self._data) |
---|
778 | |
---|
779 | if extrapolation is None: |
---|
780 | return self._qstar |
---|
781 | |
---|
782 | # Compute invariant plus invariant of extrapolated data |
---|
783 | extrapolation = extrapolation.lower() |
---|
784 | if extrapolation == "low": |
---|
785 | qs_low, dqs_low = self.get_qstar_low() |
---|
786 | qs_hi, dqs_hi = 0, 0 |
---|
787 | |
---|
788 | elif extrapolation == "high": |
---|
789 | qs_low, dqs_low = 0, 0 |
---|
790 | qs_hi, dqs_hi = self.get_qstar_high() |
---|
791 | |
---|
792 | elif extrapolation == "both": |
---|
793 | qs_low, dqs_low = self.get_qstar_low() |
---|
794 | qs_hi, dqs_hi = self.get_qstar_high() |
---|
795 | |
---|
796 | self._qstar += qs_low + qs_hi |
---|
797 | self._qstar_err = math.sqrt(self._qstar_err*self._qstar_err \ |
---|
798 | + dqs_low*dqs_low + dqs_hi*dqs_hi) |
---|
799 | |
---|
800 | return self._qstar |
---|
801 | |
---|
802 | def get_surface(self, contrast, porod_const, extrapolation=None): |
---|
803 | """ |
---|
804 | Compute the specific surface from the data. |
---|
805 | |
---|
806 | Implementation:: |
---|
807 | |
---|
808 | V = self.get_volume_fraction(contrast, extrapolation) |
---|
809 | |
---|
810 | Compute the surface given by: |
---|
811 | surface = (2*pi *V(1- V)*porod_const)/ q_star |
---|
812 | |
---|
813 | :param contrast: contrast value to compute the volume |
---|
814 | :param porod_const: Porod constant to compute the surface |
---|
815 | :param extrapolation: string to apply optional extrapolation |
---|
816 | |
---|
817 | :return: specific surface |
---|
818 | """ |
---|
819 | # Compute the volume |
---|
820 | volume = self.get_volume_fraction(contrast, extrapolation) |
---|
821 | return 2 * math.pi * volume *(1 - volume) * \ |
---|
822 | float(porod_const)/self._qstar |
---|
823 | |
---|
824 | def get_volume_fraction(self, contrast, extrapolation=None): |
---|
825 | """ |
---|
826 | Compute volume fraction is deduced as follow: :: |
---|
827 | |
---|
828 | q_star = 2*(pi*contrast)**2* volume( 1- volume) |
---|
829 | for k = 10^(-8)*q_star/(2*(pi*|contrast|)**2) |
---|
830 | we get 2 values of volume: |
---|
831 | with 1 - 4 * k >= 0 |
---|
832 | volume1 = (1- sqrt(1- 4*k))/2 |
---|
833 | volume2 = (1+ sqrt(1- 4*k))/2 |
---|
834 | |
---|
835 | q_star: the invariant value included extrapolation is applied |
---|
836 | unit 1/A^(3)*1/cm |
---|
837 | q_star = self.get_qstar() |
---|
838 | |
---|
839 | the result returned will be 0 <= volume <= 1 |
---|
840 | |
---|
841 | :param contrast: contrast value provides by the user of type float. |
---|
842 | contrast unit is 1/A^(2)= 10^(16)cm^(2) |
---|
843 | :param extrapolation: string to apply optional extrapolation |
---|
844 | |
---|
845 | :return: volume fraction |
---|
846 | |
---|
847 | :note: volume fraction must have no unit |
---|
848 | """ |
---|
849 | if contrast <= 0: |
---|
850 | raise ValueError, "The contrast parameter must be greater than zero" |
---|
851 | |
---|
852 | # Make sure Q star is up to date |
---|
853 | self.get_qstar(extrapolation) |
---|
854 | |
---|
855 | if self._qstar <= 0: |
---|
856 | msg = "Invalid invariant: Invariant Q* must be greater than zero" |
---|
857 | raise RuntimeError, msg |
---|
858 | |
---|
859 | # Compute intermediate constant |
---|
860 | k = 1.e-8 * self._qstar/(2 * (math.pi * math.fabs(float(contrast)))**2) |
---|
861 | # Check discriminant value |
---|
862 | discrim = 1 - 4 * k |
---|
863 | |
---|
864 | # Compute volume fraction |
---|
865 | if discrim < 0: |
---|
866 | msg = "Could not compute the volume fraction: negative discriminant" |
---|
867 | raise RuntimeError, msg |
---|
868 | elif discrim == 0: |
---|
869 | return 1/2 |
---|
870 | else: |
---|
871 | volume1 = 0.5 * (1 - math.sqrt(discrim)) |
---|
872 | volume2 = 0.5 * (1 + math.sqrt(discrim)) |
---|
873 | |
---|
874 | if 0 <= volume1 and volume1 <= 1: |
---|
875 | return volume1 |
---|
876 | elif 0 <= volume2 and volume2 <= 1: |
---|
877 | return volume2 |
---|
878 | msg = "Could not compute the volume fraction: inconsistent results" |
---|
879 | raise RuntimeError, msg |
---|
880 | |
---|
881 | def get_qstar_with_error(self, extrapolation=None): |
---|
882 | """ |
---|
883 | Compute the invariant uncertainty. |
---|
884 | This uncertainty computation depends on whether or not the data is |
---|
885 | smeared. |
---|
886 | |
---|
887 | :param extrapolation: string to apply optional extrapolation |
---|
888 | |
---|
889 | :return: invariant, the invariant uncertainty |
---|
890 | """ |
---|
891 | self.get_qstar(extrapolation) |
---|
892 | return self._qstar, self._qstar_err |
---|
893 | |
---|
894 | def get_volume_fraction_with_error(self, contrast, extrapolation=None): |
---|
895 | """ |
---|
896 | Compute uncertainty on volume value as well as the volume fraction |
---|
897 | This uncertainty is given by the following equation: :: |
---|
898 | |
---|
899 | dV = 0.5 * (4*k* dq_star) /(2* math.sqrt(1-k* q_star)) |
---|
900 | |
---|
901 | for k = 10^(-8)*q_star/(2*(pi*|contrast|)**2) |
---|
902 | |
---|
903 | q_star: the invariant value including extrapolated value if existing |
---|
904 | dq_star: the invariant uncertainty |
---|
905 | dV: the volume uncertainty |
---|
906 | |
---|
907 | The uncertainty will be set to -1 if it can't be computed. |
---|
908 | |
---|
909 | :param contrast: contrast value |
---|
910 | :param extrapolation: string to apply optional extrapolation |
---|
911 | |
---|
912 | :return: V, dV = volume fraction, error on volume fraction |
---|
913 | """ |
---|
914 | volume = self.get_volume_fraction(contrast, extrapolation) |
---|
915 | |
---|
916 | # Compute error |
---|
917 | k = 1.e-8 * self._qstar /(2 * (math.pi* math.fabs(float(contrast)))**2) |
---|
918 | # Check value inside the sqrt function |
---|
919 | value = 1 - k * self._qstar |
---|
920 | if (value) <= 0: |
---|
921 | uncertainty = -1 |
---|
922 | # Compute uncertainty |
---|
923 | uncertainty = math.fabs((0.5 * 4 * k * \ |
---|
924 | self._qstar_err)/(2 * math.sqrt(1 - k * self._qstar))) |
---|
925 | |
---|
926 | return volume, uncertainty |
---|
927 | |
---|
928 | def get_surface_with_error(self, contrast, porod_const, extrapolation=None): |
---|
929 | """ |
---|
930 | Compute uncertainty of the surface value as well as the surface value. |
---|
931 | The uncertainty is given as follow: :: |
---|
932 | |
---|
933 | dS = porod_const *2*pi[( dV -2*V*dV)/q_star |
---|
934 | + dq_star(v-v**2) |
---|
935 | |
---|
936 | q_star: the invariant value |
---|
937 | dq_star: the invariant uncertainty |
---|
938 | V: the volume fraction value |
---|
939 | dV: the volume uncertainty |
---|
940 | |
---|
941 | :param contrast: contrast value |
---|
942 | :param porod_const: porod constant value |
---|
943 | :param extrapolation: string to apply optional extrapolation |
---|
944 | |
---|
945 | :return S, dS: the surface, with its uncertainty |
---|
946 | """ |
---|
947 | # We get the volume fraction, with error |
---|
948 | # get_volume_fraction_with_error calls get_volume_fraction |
---|
949 | # get_volume_fraction calls get_qstar |
---|
950 | # which computes Qstar and dQstar |
---|
951 | v, dv = self.get_volume_fraction_with_error(contrast, extrapolation) |
---|
952 | |
---|
953 | s = self.get_surface(contrast=contrast, porod_const=porod_const, |
---|
954 | extrapolation=extrapolation) |
---|
955 | ds = porod_const * 2 * math.pi * (( dv - 2 * v * dv)/ self._qstar\ |
---|
956 | + self._qstar_err * ( v - v**2)) |
---|
957 | |
---|
958 | return s, ds |
---|