| Hayter Msa |
# Note: model title and parameter table are inserted automatically Calculates the interparticle structure factor for a system of charged, spheroidal, objects in a dielectric medium [1,2]. When comb... |
Structure Factor |
07 Sep 2017 |
sasview |
0 |
|
| Broad Peak |
Definition
This model calculates an empirical functional form for SAS data characterized by a broad scattering peak. Many SAS spectra are characterized by a broad peak even though they are fr... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| Multilayer Vesicle |
Definition
This model is a trivial extension of the core_shell_sphere function where the core is filled with solvent and is surrounded by $N$ shells of material (such as lipids) interleaved w... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Stickyhardsphere |
# Note: model title and parameter table are inserted automatically Calculates the interparticle structure factor for a hard sphere fluid with a narrow, attractive, potential well. Unlike the `squar... |
Structure Factor |
07 Sep 2017 |
sasview |
0 |
|
| Spherical Sld |
Definition
Similarly to the onion, this model provides the form factor, $P(q)$, for a multi-shell sphere, where the interface between the each neighboring shells can be described by the error... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Gauss Lorentz Gel |
This model calculates the scattering from a gel structure, but typically a physical rather than chemical network. It is modeled as a sum of a low-q exponential decay (which happens to give a functi... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| Core Shell Bicelle Elliptical |
Definition
This model provides the form factor for an elliptical cylinder with a core-shell scattering length density profile [#Onsager1949]_. Thus this is a variation of the core-shell bicel... |
Cylinder |
07 Sep 2017 |
sasview |
0 |
|
| Triaxial Ellipsoid |
# triaxial ellipsoid model # Note: model title and parameter table are inserted automatically Definition
Ellipsoid with $R_a$ as *radius_equat_minor*, $R_b$ as *radius_equat_major* ... |
Ellipsoid |
07 Sep 2017 |
sasview |
0 |
|
| Adsorbed Layer |
Definition
This model describes the scattering from a layer of surfactant or polymer adsorbed on large, smooth, notionally spherical particles under the conditions that (i) the particles (cor... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Two Lorentzian |
Definition
The scattering intensity $I(q)$ is calculated as
$$ I(q) = \frac{A}{1 +(Q\xi_1)^n} + \frac{C}{1 +(Q\xi_2)^m} + \text{B}
$$
where $A$ = Lorentzian scale factor #1, $C$ = Lorent... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| Vesicle |
Definition
This model provides the form factor, *P(q)*, for an unilamellar vesicle and is effectively identical to the hollow sphere reparameterized to be more intuitive for a vesicle and nor... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Surface Fractal |
This model calculates the scattering from fractal-like aggregates based on the Mildner reference.
Definition
The scattering intensity $I(q)$ is calculated as
$$ \begin{align*} I(q) = \... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| Core Multi Shell |
Definition
This model is a trivial extension of the CoreShell function to a larger number of shells. The scattering length density profile for the default sld values (w/ 4 shells).
... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Core Shell Sphere |
.. _core_shell_sphere:
This model provides the form factor, $P(q)$, for a spherical particle with a core-shell structure. The form factor is normalized by the particle volume.
For information... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Hollow Rectangular Prism Thin Walls |
# rectangular_prism model # Note: model title and parameter table are inserted automatically Definition
This model provides the form factor, $P(q)$, for a hollow rectangular prism with infinitel... |
Parallelepiped |
07 Sep 2017 |
sasview |
0 |
|
| Mono Gauss Coil |
#mono_gauss_coil model #conversion of DebyeModel.py #converted by Steve King, Mar 2016 This Debye Gaussian coil model strictly describes the scattering from *monodisperse* polymer chains in theta s... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| Elliptical Cylinder |
# pylint: disable=line-too-long
Elliptical cylinder geometry $a = r_\text{minor}$ and $\nu = r_\text{major} / r_\text{minor}$ is the *axis_ratio*.
The function calculated is
$$ I... |
Cylinder |
07 Sep 2017 |
sasview |
0 |
|
| Fuzzy Sphere |
For information about polarised and magnetic scattering, see the `magnetism` documentation.
Definition
Scattering from spheres with a Gaussian interface.
The scattering intensity $I(q)$... |
Sphere |
07 Sep 2017 |
sasview |
0 |
|
| Porod |
This model is a special case of the power law model, deriving its special name from the Porod Law which it models, where the power law exponent is fixed to -4.
$$ I(q) = C/q^4 + Background
$$
W... |
Shape-Independent |
07 Sep 2017 |
sasview |
0 |
|
| star_polymer_v2 |
Reparametrised version, fits Rg not Rg^2^
Documentation corrected, see ticket #962, with grateful thanks to Ziang Li for pointing out the issues.
The models is still noisy at very small Q when Rg... |
Shape-Independent |
22 May 2017 |
richardh |
0 |
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