source: sasmodels/sasmodels/models/spherical_sld.py @ 50ec515

r"""
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 function, power-law, or exponential
functions.  The scattering intensity is computed by building a continuous
custom SLD profile along the radius of the particle. The SLD profile is
composed of a number of uniform shells with interfacial shells between them.

.. figure:: img/spherical_sld_profile.png

    Example SLD profile

Unlike the <onion> model (using an analytical integration), the interfacial
shells here are sub-divided and numerically integrated assuming each
sub-shell is described by a line function, with *n_steps* sub-shells per
interface. The form factor is normalized by the total volume of the sphere.

Interface shapes are as follows::

    0: erf(|nu|*z)
    1: Rpow(z^|nu|)
    2: Lpow(z^|nu|)
    3: Rexp(-|nu|z)
    4: Lexp(-|nu|z)

Definition
----------

The form factor $P(q)$ in 1D is calculated by:

.. math::

    P(q) = \frac{f^2}{V_\text{particle}} \text{ where }
    f = f_\text{core} + \sum_{\text{inter}_i=0}^N f_{\text{inter}_i} +
    \sum_{\text{flat}_i=0}^N f_{\text{flat}_i} +f_\text{solvent}

For a spherically symmetric particle with a particle density $\rho_x(r)$
the sld function can be defined as:

.. math::

    f_x = 4 \pi \int_{0}^{\infty} \rho_x(r)  \frac{\sin(qr)} {qr^2} r^2 dr


so that individual terms can be calculated as follows:

.. math::
    f_\text{core} = 4 \pi \int_{0}^{r_\text{core}} \rho_\text{core}
    \frac{\sin(qr)} {qr} r^2 dr =
    3 \rho_\text{core} V(r_\text{core})
    \Big[ \frac{\sin(qr_\text{core}) - qr_\text{core} \cos(qr_\text{core})}
    {qr_\text{core}^3} \Big]

    f_{\text{inter}_i} = 4 \pi \int_{\Delta t_{ \text{inter}_i } }
    \rho_{ \text{inter}_i } \frac{\sin(qr)} {qr} r^2 dr

    f_{\text{shell}_i} = 4 \pi \int_{\Delta t_{ \text{inter}_i } }
    \rho_{ \text{flat}_i } \frac{\sin(qr)} {qr} r^2 dr =
    3 \rho_{ \text{flat}_i } V ( r_{ \text{inter}_i } +
    \Delta t_{ \text{inter}_i } )
    \Big[ \frac{\sin(qr_{\text{inter}_i} + \Delta t_{ \text{inter}_i } )
    - q (r_{\text{inter}_i} + \Delta t_{ \text{inter}_i })
    \cos(q( r_{\text{inter}_i} + \Delta t_{ \text{inter}_i } ) ) }
    {q ( r_{\text{inter}_i} + \Delta t_{ \text{inter}_i } )^3 }  \Big]
    -3 \rho_{ \text{flat}_i } V(r_{ \text{inter}_i })
    \Big[ \frac{\sin(qr_{\text{inter}_i}) - qr_{\text{flat}_i}
    \cos(qr_{\text{inter}_i}) } {qr_{\text{inter}_i}^3} \Big]

    f_\text{solvent} = 4 \pi \int_{r_N}^{\infty} \rho_\text{solvent}
    \frac{\sin(qr)} {qr} r^2 dr =
    3 \rho_\text{solvent} V(r_N)
    \Big[ \frac{\sin(qr_N) - qr_N \cos(qr_N)} {qr_N^3} \Big]


Here we assumed that the SLDs of the core and solvent are constant in $r$.
The SLD at the interface between shells, $\rho_{\text {inter}_i}$
is calculated with a function chosen by an user, where the functions are

Exp:

.. math::
    \rho_{{inter}_i} (r) = \begin{cases}
    B \exp\Big( \frac {\pm A(r - r_{\text{flat}_i})}
    {\Delta t_{ \text{inter}_i }} \Big) +C  & \text{for} A \neq 0 \\
    B \Big( \frac {(r - r_{\text{flat}_i})}
    {\Delta t_{ \text{inter}_i }} \Big) +C  & \text{for} A = 0 \\
    \end{cases}

Power-Law

.. math::
    \rho_{{inter}_i} (r) = \begin{cases}
    \pm B \Big( \frac {(r - r_{\text{flat}_i} )} {\Delta t_{ \text{inter}_i }}
    \Big) ^A  +C  & \text{for} A \neq 0 \\
    \rho_{\text{flat}_{i+1}}  & \text{for} A = 0 \\
    \end{cases}

Erf:

.. math::
    \rho_{{inter}_i} (r) = \begin{cases}
    B \text{erf} \Big( \frac { A(r - r_{\text{flat}_i})}
    {\sqrt{2} \Delta t_{ \text{inter}_i }} \Big) +C  & \text{for} A \neq 0 \\
    B \Big( \frac {(r - r_{\text{flat}_i} )} {\Delta t_{ \text{inter}_i }}
    \Big)  +C  & \text{for} A = 0 \\
    \end{cases}

The functions are normalized so that they vary between 0 and 1, and they are
constrained such that the SLD is continuous at the boundaries of the interface
as well as each sub-shell. Thus B and C are determined.

Once $\rho_{\text{inter}_i}$ is found at the boundary of the sub-shell of the
interface, we can find its contribution to the form factor $P(q)$

.. math::
    f_{\text{inter}_i} = 4 \pi \int_{\Delta t_{ \text{inter}_i } }
    \rho_{ \text{inter}_i } \frac{\sin(qr)} {qr} r^2 dr =
    4 \pi \sum_{j=0}^{npts_{\text{inter}_i} -1 }
    \int_{r_j}^{r_{j+1}} \rho_{ \text{inter}_i } (r_j)
    \frac{\sin(qr)} {qr} r^2 dr \approx

    4 \pi \sum_{j=0}^{npts_{\text{inter}_i} -1 } \Big[
    3 ( \rho_{ \text{inter}_i } ( r_{j+1} ) - \rho_{ \text{inter}_i }
    ( r_{j} ) V ( r_{ \text{subshell}_j } )
    \Big[ \frac {r_j^2 \beta_\text{out}^2 \sin(\beta_\text{out})
    - (\beta_\text{out}^2-2) \cos(\beta_\text{out}) }
    {\beta_\text{out}^4 } \Big]

    - 3 ( \rho_{ \text{inter}_i } ( r_{j+1} ) - \rho_{ \text{inter}_i }
    ( r_{j} ) V ( r_{ \text{subshell}_j-1 } )
    \Big[ \frac {r_{j-1}^2 \sin(\beta_\text{in})
    - (\beta_\text{in}^2-2) \cos(\beta_\text{in}) }
    {\beta_\text{in}^4 } \Big]

    + 3 \rho_{ \text{inter}_i } ( r_{j+1} )  V ( r_j )
    \Big[ \frac {\sin(\beta_\text{out}) - \cos(\beta_\text{out}) }
    {\beta_\text{out}^4 } \Big]

    - 3 \rho_{ \text{inter}_i } ( r_{j} )  V ( r_j )
    \Big[ \frac {\sin(\beta_\text{in}) - \cos(\beta_\text{in}) }
    {\beta_\text{in}^4 } \Big]
    \Big]

where

.. math::
    V(a) = \frac {4\pi}{3}a^3

    a_\text{in} ~ \frac{r_j}{r_{j+1} -r_j} \text{, } a_\text{out}
    ~ \frac{r_{j+1}}{r_{j+1} -r_j}

    \beta_\text{in} = qr_j \text{, } \beta_\text{out} = qr_{j+1}


We assume $\rho_{\text{inter}_j} (r)$ is approximately linear
within the sub-shell $j$.

Finally the form factor can be calculated by

.. math::

    P(q) = \frac{[f]^2} {V_\text{particle}} \text{where} V_\text{particle}
    = V(r_{\text{shell}_N})

For 2D data the scattering intensity is calculated in the same way as 1D,
where the $q$ vector is defined as

.. math::

    q = \sqrt{q_x^2 + q_y^2}

.. note::

    The outer most radius is used as the effective radius for S(Q)
    when $P(Q) * S(Q)$ is applied.

References
----------
L A Feigin and D I Svergun, Structure Analysis by Small-Angle X-Ray
and Neutron Scattering, Plenum Press, New York, (1987)

"""

import numpy as np
from numpy import inf, expm1, sqrt
from scipy.special import erf

name = "spherical_sld"
title = "Sperical SLD intensity calculation"
description = """
            I(q) =
               background = Incoherent background [1/cm]
        """
category = "shape:sphere"

SHAPES = [["erf(|nu|*z)", "Rpow(z^|nu|)", "Lpow(z^|nu|)",
           "Rexp(-|nu|z)", "Lexp(-|nu|z)"]]

# pylint: disable=bad-whitespace, line-too-long
#            ["name", "units", default, [lower, upper], "type", "description"],
parameters = [["n_shells",             "",           1,      [1, 10],        "volume", "number of shells"],
              ["sld_solvent",          "1e-6/Ang^2", 1.0,    [-inf, inf],    "sld", "solvent sld"],
              ["sld[n_shells]",        "1e-6/Ang^2", 4.06,   [-inf, inf],    "sld", "sld of the shell"],
              ["thickness[n_shells]",  "Ang",        100.0,  [0, inf],       "volume", "thickness shell"],
              ["interface[n_shells]",  "Ang",        50.0,   [0, inf],       "volume", "thickness of the interface"],
              ["shape[n_shells]",      "",           0,      SHAPES,         "", "interface shape"],
              ["nu[n_shells]",         "",           2.5,    [0, inf],       "", "interface shape exponent"],
              ["n_steps",              "",           35,     [0, inf],       "", "number of steps in each interface (must be an odd integer)"],
              ]
# pylint: enable=bad-whitespace, line-too-long
source = ["lib/polevl.c", "lib/sas_erf.c", "lib/sph_j1c.c", "spherical_sld.c"]
single = False  # TODO: fix low q behaviour

profile_axes = ['Radius (A)', 'SLD (1e-6/A^2)']

SHAPE_FUNCTIONS = [
    lambda z, nu: erf(nu/sqrt(2)*(2*z-1))/(2*erf(nu/sqrt(2))) + 0.5,  # erf
    lambda z, nu: z**nu,                    # Rpow
    lambda z, nu: 1 - (1-z)**nu,            # Lpow
    lambda z, nu: expm1(-nu*z)/expm1(-nu),  # Rexp
    lambda z, nu: expm1(nu*z)/expm1(nu),    # Lexp
]

def profile(n_shells, sld_solvent, sld, thickness,
            interface, shape, nu, n_steps):
    """
    Returns shape profile with x=radius, y=SLD.
    """

    z = []
    rho = []
    z0 = 0
    # two sld points for core
    z.append(0)
    rho.append(sld[0])

    for i in range(0, int(n_shells)):
        z0 += thickness[i]
        z.append(z0)
        rho.append(sld[i])
        dz = interface[i]/n_steps
        sld_l = sld[i]
        sld_r = sld[i+1] if i < n_shells-1 else sld_solvent
        fn = SHAPE_FUNCTIONS[int(np.clip(shape[i], 0, len(SHAPE_FUNCTIONS)-1))]
        for step in range(1, n_steps+1):
            portion = fn(float(step)/n_steps, max(abs(nu[i]), 1e-14))
            z0 += dz
            z.append(z0)
            rho.append((sld_r - sld_l)*portion + sld_l)
    z.append(z0*1.2)
    rho.append(sld_solvent)
    # return sld profile (r, beta)
    return np.asarray(z), np.asarray(rho)


def ER(n_shells, thickness, interface):
    n_shells = int(n_shells)
    total = (np.sum(thickness[:n_shells], axis=1)
             + np.sum(interface[:n_shells], axis=1))
    return total


demo = {
    "n_shells": 5,
    "n_steps": 35.0,
    "sld_solvent": 1.0,
    "sld":[2.07,4.0,3.5,4.0,3.5],
    "thickness":[50.0,100.0,100.0,100.0,100.0],
    "interface":[50.0,50.0,50.0,50.0],
    "shape": [0,0,0,0,0],
    "nu":[2.5,2.5,2.5,2.5,2.5],
    }

#TODO: Not working yet
"""
tests = [
    # Accuracy tests based on content in test/utest_extra_models.py
    [{"n_shells": 5,
        "n_steps": 35,
        "sld_solvent": 1.0,
        "sld": [2.07, 4.0, 3.5, 4.0, 3.5],
        "thickness": [50.0, 100.0, 100.0, 100.0, 100.0],
        "interface": [50]*5,
        "shape": [0]*5,
        "nu": [2.5]*5,
    }, 0.001, 0.001],
]
"""