1 | .. _lamellarPC: |
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2 | |
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3 | Lamellarpc |
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4 | ======================================================= |
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5 | |
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6 | Random lamellar sheet with paracrystal structure factor |
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7 | |
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8 | ================ ================================= ============ ============= |
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9 | Parameter Description Units Default value |
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10 | ================ ================================= ============ ============= |
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11 | scale Source intensity None 1 |
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12 | background Source background |cm^-1| 0 |
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13 | thickness sheet thickness |Ang| 33 |
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14 | Nlayers Number of layers None 20 |
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15 | spacing d-spacing of paracrystal stack |Ang| 250 |
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16 | spacing_polydisp d-spacing of paracrystal stack |Ang| 0 |
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17 | sld layer scattering length density |1e-6Ang^-2| 1 |
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18 | solvent_sld Solvent scattering length density |1e-6Ang^-2| 6.34 |
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19 | ================ ================================= ============ ============= |
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20 | |
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21 | The returned value is scaled to units of |cm^-1|. |
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22 | |
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23 | |
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24 | This model calculates the scattering from a stack of repeating lamellar |
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25 | structures. The stacks of lamellae (infinite in lateral dimension) are |
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26 | treated as a paracrystal to account for the repeating spacing. The repeat |
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27 | distance is further characterized by a Gaussian polydispersity. **This model |
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28 | can be used for large multilamellar vesicles.** |
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29 | |
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30 | *2.1.33.1. Definition* |
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31 | |
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32 | The scattering intensity *I(q)* is calculated as |
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33 | |
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34 | .. image:: img/image145.jpg |
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35 | |
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36 | The form factor of the bilayer is approximated as the cross section of an |
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37 | infinite, planar bilayer of thickness *t* |
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38 | |
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39 | .. image:: img/image146.jpg |
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40 | |
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41 | Here, the scale factor is used instead of the mass per area of the |
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42 | bilayer (*G*). The scale factor is the volume fraction of the material in |
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43 | the bilayer, *not* the total excluded volume of the paracrystal. |
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44 | *Z*\ :sub:`N`\ *(q)* describes the interference effects for aggregates |
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45 | consisting of more than one bilayer. The equations used are (3-5) |
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46 | from the Bergstrom reference below. |
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47 | |
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48 | Non-integer numbers of stacks are calculated as a linear combination of |
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49 | the lower and higher values |
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50 | |
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51 | .. image:: img/image147.jpg |
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52 | |
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53 | The 2D scattering intensity is the same as 1D, regardless of the orientation |
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54 | of the *q* vector which is defined as |
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55 | |
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56 | .. math:: |
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57 | |
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58 | Q = \sqrt{Q_x^2 + Q_y^2} |
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59 | |
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60 | The parameters of the model are *Nlayers* = no. of layers, and |
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61 | *pd_spacing* = polydispersity of spacing. |
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62 | |
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63 | ============== ======== ============= |
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64 | Parameter name Units Default value |
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65 | ============== ======== ============= |
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66 | background |cm^-1| 0 |
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67 | scale None 1 |
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68 | Nlayers None 20 |
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69 | pd_spacing None 0.2 |
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70 | sld_layer |Ang^-2| 1e-6 |
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71 | sld_solvent |Ang^-2| 6.34e-6 |
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72 | spacing |Ang| 250 |
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73 | thickness |Ang| 33 |
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74 | ============== ======== ============= |
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75 | |
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76 | .. image:: img/image148.jpg |
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77 | |
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78 | *Figure. 1D plot using the default values above (w/20000 data point).* |
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79 | |
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80 | Our model uses the form factor calculations implemented in a C library |
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81 | provided by the NIST Center for Neutron Research (Kline, 2006). |
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82 | |
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83 | REFERENCE |
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84 | |
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85 | M Bergstrom, J S Pedersen, P Schurtenberger, S U Egelhaaf, |
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86 | *J. Phys. Chem. B*, 103 (1999) 9888-9897 |
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87 | |
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88 | |
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