1 | Release Notes |
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2 | ============= |
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3 | |
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4 | SANS Models version 0.4.3 |
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5 | |
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6 | Package name: sans.models |
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7 | |
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8 | 1- What's New in Version 0.4.3 |
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9 | - Release date: April 21, 2009 |
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10 | - C extension models now use new C++ classes that incorporate dispersity and averaging |
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11 | functionality. See utest_dispersity.py for examples of how to use the new dispersion |
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12 | classes. |
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13 | |
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14 | # Create a model |
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15 | model= CylinderModel() |
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16 | |
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17 | # Create a dispersion model |
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18 | disp = GaussianDispersion() |
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19 | |
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20 | # Set the dispersion for a chosen parameter |
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21 | model.set_dispersion('radius', disp) |
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22 | |
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23 | # Set the parameters of the dispersion model |
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24 | model.dispersion['radius']['width'] = 5.0 |
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25 | model.dispersion['radius']['npts'] = 100 |
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26 | |
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27 | |
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28 | Version 0.4.3 |
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29 | -P(Q)*S(Q) added for P(Q)=cylinder, sphere, ellipsoid |
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30 | -Array dispersion (user defined) added |
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31 | |
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32 | Version 0.4.2 |
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33 | -4 Structure factors added |
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34 | |
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35 | Version 0.4.1 |
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36 | - Release date: 6/9/2008 |
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37 | - Modified non-shape models so that the 2D output is the 1D output for the length of Q |
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38 | |
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39 | Version 0.4.0 |
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40 | - Release date: 4/15/2008 |
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41 | - Added shape-independent models. |
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42 | |
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43 | Version 0.3.2: |
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44 | - Release date: 2/14/2008 |
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45 | - Added models to be used in magnetic analysis. |
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46 | |
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47 | |
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48 | 2- Downloading and Installing |
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49 | |
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50 | 2.1- System Requirements: |
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51 | - Python version >= 2.5 and < 3.0 should be running on the system |
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52 | |
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53 | |
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54 | 2.2- Installing: |
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55 | - Get the code from svn://danse.us/sans/releases/sansmodels-0.4.3 |
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56 | - Execute the following: |
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57 | python setup.py install |
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58 | |
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59 | 3- Known Issues |
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60 | |
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61 | 3.1- All systems: |
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62 | - Q range validity of I(q) calculations. |
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63 | Our 1D models of I(q) use the function of the NCNR library |
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64 | for their IGOR package (Klein, 2006). That library uses a |
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65 | fast integration technique in some of its models (cylinders |
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66 | and ellipsoids). Integration is done using 76 points in the |
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67 | angle between the axis of the object and the q-vector, which |
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68 | translates in a larger inaccuracy at high q. Integratiing |
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69 | the 2D model I(q,phi) over all orientations of the object |
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70 | will not yield the exact same result as the NCNR calculation |
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71 | for q > 0.3 A-1. |
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72 | - Refactoring needs to be done to update the model base class. |
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73 | We should get rid of the useless arithmetics and store the parameters |
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74 | as class objects rather than values. This would eliminate the multitude |
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75 | of dictionaries needed to store all the various aspects of a parameter |
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76 | (limits, units, dispersity information). The C++ design it relies |
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77 | on is much cleaner in that respect, but it still depends on the old |
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78 | C computation. Those should be incorporated in the C++ classes. |
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79 | |
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80 | 3.2- Windows: |
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81 | - None |
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82 | |
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83 | 3.3- Linux: |
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84 | - None |
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85 | |
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86 | 4- Troubleshooting |
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87 | |
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88 | - None |
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89 | |
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90 | 5- Frequently Asked Questions |
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91 | |
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92 | - None |
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93 | |
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94 | 6- Other Resources |
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95 | |
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96 | - See: http://danse.us/trac/sans/wiki/8_2_2_1DModelFitting |
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97 | - See: http://danse.us/trac/sans/wiki/8_2_3_2DModeling |
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98 | - See: http://danse.us/trac/sans/wiki/8_2_6_model_extensions |
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99 | - See: http://danse.us/trac/sans/wiki/8_2_1Nonshape_models |
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100 | |
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101 | |
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102 | |
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103 | |
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104 | |
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105 | |
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