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  • sasmodels/models/vesicle.py

    r216fa6d rfa8011eb  
    2424is a flat background level (due for example to incoherent scattering in the 
    2525case of neutrons), and $j_1$ is the spherical bessel function 
    26 $j_1 = (sin(x) - x cos(x))/ x^2$. 
     26$j_1 = (\sin(x) - x \cos(x))/ x^2$. 
    2727 
    2828The functional form is identical to a "typical" core-shell structure, except 
     
    3535thickness = $R_{\text{tot}} - R_{\text{core}}$. 
    3636 
    37 .. figure: img/vesicle_geometry.jpg 
     37.. figure:: img/vesicle_geometry.jpg 
     38 
     39    Vesicle geometry. 
    3840 
    3941The 2D scattering intensity is the same as *P(q)* above, regardless of the 
     
    4850radius for *S(Q)* when *P(Q)* \* *S(Q)* is applied. 
    4951 
    50 .. image:: img/vesicle_1d.jpg 
     52.. figure:: img/vesicle_1d.jpg 
    5153 
    52 *Figure. 1D plot using the default values given in the table 
    53 (w/200 data point). Polydispersity and instrumental resolution normally 
    54 will smear out most of the rapidly oscillating features.* 
     54    1D plot using the default values given in the table (w/200 data point). 
     55    Polydispersity and instrumental resolution normally will smear out most 
     56    of the rapidly oscillating features. 
    5557 
    5658REFERENCE 
     
    6062""" 
    6163 
    62 import numpy as np 
    6364from numpy import pi, inf 
    6465 
     
    131132# NOTE: test results taken from values returned by SasView 3.1.2 
    132133tests = [[{}, 0.0010005303255, 17139.8268799], 
    133          [{}, 0.200027832249, 0.130387268704 ], 
     134         [{}, 0.200027832249, 0.130387268704], 
    134135         [{}, 'ER', 130.], 
    135136         [{}, 'VR', 0.54483386436], 
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