1 | r""" |
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2 | Definition |
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3 | ---------- |
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4 | |
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5 | This model calculates an empirical functional form for SAS data characterized |
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6 | by a broad scattering peak. Many SAS spectra are characterized by a broad peak |
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7 | even though they are from amorphous soft materials. For example, soft systems |
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8 | that show a SAS peak include copolymers, polyelectrolytes, multiphase systems, |
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9 | layered structures, etc. |
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10 | |
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11 | The d-spacing corresponding to the broad peak is a characteristic distance |
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12 | between the scattering inhomogeneities (such as in lamellar, cylindrical, or |
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13 | spherical morphologies, or for bicontinuous structures). |
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14 | |
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15 | The scattering intensity $I(q)$ is calculated as |
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16 | |
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17 | .. math:: I(q) = \frac{A}{q^n} + \frac{C}{1 + (|q - q_0|\xi)^m} + B |
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18 | |
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19 | Here the peak position is related to the d-spacing as $q_0 = 2\pi / d_0$. |
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20 | |
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21 | $A$ is the Porod law scale factor, $n$ the Porod exponent, $C$ is the |
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22 | Lorentzian scale factor, $m$ the exponent of $q$, $\xi$ the screening length, |
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23 | and $B$ the flat background. |
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24 | |
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25 | For 2D data the scattering intensity is calculated in the same way as 1D, |
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26 | where the $q$ vector is defined as |
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27 | |
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28 | .. math:: q = \sqrt{q_x^2 + q_y^2} |
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29 | |
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30 | References |
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31 | ---------- |
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32 | |
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33 | None. |
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34 | |
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35 | Authorship and Verification |
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36 | ---------------------------- |
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37 | |
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38 | * **Author:** NIST IGOR/DANSE **Date:** pre 2010 |
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39 | * **Last Modified by:** Paul kienle **Date:** July 24, 2016 |
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40 | * **Last Reviewed by:** Richard Heenan **Date:** March 21, 2016 |
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41 | """ |
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42 | |
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43 | from numpy import inf, errstate |
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44 | |
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45 | name = "broad_peak" |
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46 | title = "Broad Lorentzian type peak on top of a power law decay" |
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47 | description = """\ |
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48 | I(q) = scale_p/pow(q,exponent)+scale_l/ |
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49 | (1.0 + pow((fabs(q-q_peak)*length_l),exponent_l) )+ background |
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50 | |
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51 | List of default parameters: |
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52 | porod_scale = Porod term scaling |
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53 | porod_exp = Porod exponent |
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54 | lorentz_scale = Lorentzian term scaling |
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55 | lorentz_length = Lorentzian screening length [A] |
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56 | peak_pos = peak location [1/A] |
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57 | lorentz_exp = Lorentzian exponent |
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58 | background = Incoherent background""" |
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59 | category = "shape-independent" |
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60 | |
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61 | # pylint: disable=bad-whitespace, line-too-long |
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62 | # ["name", "units", default, [lower, upper], "type", "description"], |
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63 | parameters = [["porod_scale", "", 1.0e-05, [-inf, inf], "", "Power law scale factor"], |
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64 | ["porod_exp", "", 3.0, [-inf, inf], "", "Exponent of power law"], |
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65 | ["lorentz_scale", "", 10.0, [-inf, inf], "", "Scale factor for broad Lorentzian peak"], |
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66 | ["lorentz_length", "Ang", 50.0, [-inf, inf], "", "Lorentzian screening length"], |
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67 | ["peak_pos", "1/Ang", 0.1, [-inf, inf], "", "Peak position in q"], |
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68 | ["lorentz_exp", "", 2.0, [-inf, inf], "", "Exponent of Lorentz function"], |
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69 | ] |
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70 | # pylint: enable=bad-whitespace, line-too-long |
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71 | |
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72 | def Iq(q, |
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73 | porod_scale=1.0e-5, |
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74 | porod_exp=3.0, |
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75 | lorentz_scale=10.0, |
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76 | lorentz_length=50.0, |
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77 | peak_pos=0.1, |
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78 | lorentz_exp=2.0): |
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79 | """ |
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80 | :param q: Input q-value |
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81 | :param porod_scale: Power law scale factor |
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82 | :param porod_exp: Exponent of power law |
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83 | :param lorentz_scale: Scale factor for broad Lorentzian peak |
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84 | :param lorentz_length: Lorentzian screening length |
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85 | :param peak_pos: Peak position in q |
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86 | :param lorentz_exp: Exponent of Lorentz function |
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87 | :return: Calculated intensity |
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88 | """ |
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89 | z = abs(q - peak_pos) * lorentz_length |
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90 | with errstate(divide='ignore'): |
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91 | inten = (porod_scale / q ** porod_exp |
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92 | + lorentz_scale / (1 + z ** lorentz_exp)) |
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93 | return inten |
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94 | Iq.vectorized = True # Iq accepts an array of q values |
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95 | |
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96 | demo = dict(scale=1, background=0, |
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97 | porod_scale=1.0e-05, porod_exp=3, |
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98 | lorentz_scale=10, lorentz_length=50, peak_pos=0.1, lorentz_exp=2) |
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