import os
os.environ["SAS_OPENCL"] = "cuda" # use CUDA GPU backend for sasmodels
import escape as esc
import numpy as np
esc.require("0.9.8")
Loading material database from C:\dev\escape-core\python\src\escape\scattering\..\data\mdb\materials.db
SAXS. Form-factors. Elliptical cylinder (SasView-aligned)¶
A right cylinder with an elliptical cross-section. The 1D powder average integrates over both the tilt angle $\alpha$ (axis vs $\mathbf{q}$) and the in-plane azimuthal angle $\psi$.
Reference: https://www.sasview.org/docs/user/models/elliptical_cylinder.html
Parameters (SasView defaults)¶
| Parameter | Variable | Value |
|---|---|---|
| Scale | scale |
1 |
| Background (cm⁻¹) | background |
0.001 |
| Minor radius (Å) | radius_minor |
20 |
| Axis ratio ν = major/minor | axis_ratio |
1.5 |
| Length (Å) | length |
400 |
| Contrast Δρ (10⁻⁶ Å⁻²) | contrast |
3 (= sld 4 − sld_solvent 1) |
| Theta (deg), 2D only | theta |
90 |
| Phi (deg), 2D only | phi |
0 |
Form-factor (SasView elliptical_cylinder.c)¶
The effective radius depends on the in-plane azimuthal angle $\psi$:
$$r'(\psi) = \frac{r_{\min}}{\sqrt{2}}\sqrt{(1+\nu^2)+(1-\nu^2)\cos\psi}$$
The oriented amplitude:
$$F(q,\alpha,\psi) = V\cdot\frac{2J_1(r'\,q_\perp)}{r'\,q_\perp}\;\mathrm{sinc}\!\left(\tfrac{L}{2}q_\parallel\right)$$
$$I(q) = \frac{\mathrm{scale}}{V}\cdot\frac{2}{\pi}\int_0^{\pi/2}d\psi\int_0^{\pi/2}F^2\,\sin\alpha\,d\alpha + \mathrm{background}$$
# ── Variables ──────────────────────────────────────────────────────────────
q = esc.var("Q")
alpha = esc.var("alpha") # tilt angle between cylinder axis and q
psi = esc.var("psi") # in-plane azimuthal angle (averages ellipse orientation)
# ── Parameters ─────────────────────────────────────────────────────────────
scale = esc.par("Scale", 1.0, scale=1e8, fixed=True)
radius_minor = esc.par("Radius minor", 20.0, units=esc.angstr)
axis_ratio = esc.par("Axis ratio", 1.5, userlim=[1.0, 10.0])
length = esc.par("Length", 400.0, units=esc.angstr)
contrast = esc.par("Contrast", 3.0, scale=1e-6, units=f"{esc.angstr}^-2")
background = esc.par("Background", 0.001, userlim=[0.0, 0.03])
# ── Geometry ───────────────────────────────────────────────────────────────
# Geometric-mean radius: r_eff = sqrt(a*b) = r_minor * sqrt(axis_ratio)
r_eff = radius_minor * esc.sqrt(axis_ratio)
volume = np.pi * esc.pow(r_eff, 2) * length
# ψ-dependent effective radius for the Bessel argument
r_psi = (radius_minor / esc.sqrt(2.0)) * esc.sqrt(
(1.0 + esc.pow(axis_ratio, 2)) + (1.0 - esc.pow(axis_ratio, 2)) * esc.cos(psi))
# ── Oriented amplitude ─────────────────────────────────────────────────────
q_axial = q * esc.cos(alpha)
q_radial = q * esc.sin(alpha)
# F = V * 2*J1(r_psi*q_radial)/(r_psi*q_radial) * sinc(L/2*q_axial)
F_psi = volume * 2.0 * esc.j1_over_x(r_psi * q_radial) * esc.sinc(0.5 * length * q_axial)
# ── Powder average: integrate over alpha then psi ──────────────────────────
# Inner integral over alpha (orientation average)
alpha_integral = esc.integral(esc.pow(F_psi, 2) * esc.sin(alpha),
alpha, 0.0, np.pi / 2.0,
numpoints=61, maxiter=5, epsabs=1e-5)
# Outer integral over psi (ellipse orientation average), normalised by 1/pi
i1d = (scale * esc.pow(contrast, 2) / volume
* esc.integral(alpha_integral, psi, 0.0, np.pi,
numpoints=61, maxiter=5, epsabs=1e-5)
* (1.0 / np.pi)
+ background)
i1d.device = "gpu"
qs = np.linspace(0.001, 1.0, 300)
i1d.show(coordinates=qs).config(
title="Elliptical cylinder — powder average (1D)",
xlog=True, ylog=True,
xlabel=f"Q [{esc.angstr}^-1]", ylabel="I(q) [cm^-1]")
2D oriented scattering (qx, qy)¶
For a fixed orientation $(\theta, \phi)$ the geometric-mean radius $r_{\mathrm{eff}} = \sqrt{ab}$ is used for the Bessel argument (the ψ average is replaced by a fixed effective radius).
$$I_{\mathrm{2D}}(q_x,q_y) = \frac{\mathrm{scale}}{V}\,F^2(q_\parallel, q_\perp) + \mathrm{background}$$
qx = esc.var("qx")
qy = esc.var("qy")
theta = esc.par("Theta", 90.0, userlim=[0.0, 180.0], units="deg")
phi = esc.par("Phi", 0.0, userlim=[0.0, 360.0], units="deg")
deg = np.pi / 180.0
sin_t = esc.sin(theta * deg)
ux = sin_t * esc.cos(phi * deg)
uy = sin_t * esc.sin(phi * deg)
q_sq = esc.pow(qx, 2) + esc.pow(qy, 2)
q_par_2d = qx * ux + qy * uy
q_perp_2d = esc.sqrt(q_sq - esc.pow(q_par_2d, 2))
# Use geometric-mean radius r_eff for the 2D oriented case
F_2d = volume * 2.0 * esc.j1_over_x(r_eff * q_perp_2d) * esc.sinc(0.5 * length * q_par_2d)
i2d = scale * esc.pow(contrast, 2) / volume * esc.pow(F_2d, 2) + background
i2d.device = "gpu"
xs = np.linspace(-1.0, 1.0, 300); ys = np.linspace(-1.0, 1.0, 300)
xv, yv = np.meshgrid(xs, ys)
coords_2d = np.column_stack([xv.flatten(), yv.flatten()]).flatten()
i2d.show(coordinates=coords_2d).config(
title="Elliptical cylinder — oriented 2D SAXS (qx, qy)",
xlabel=f"qx [{esc.angstr}^-1]", ylabel=f"qy [{esc.angstr}^-1]",
cblog=True, colorscale="jet")
SasView reference model & comparison¶
| ESCAPE parameter | SasView parameter | Notes |
|---|---|---|
contrast * 1e-6 |
sld - sld_solvent |
contrast in Å⁻² |
radius_minor |
r_minor |
minor semi-axis (Å) |
axis_ratio |
r_ratio |
major/minor ratio |
length |
length |
cylinder length (Å) |
import time
import matplotlib.pyplot as plt
from sasmodels.core import load_model
from sasmodels.data import empty_data1D
from sasmodels.direct_model import DirectModel
qs = np.linspace(0.001, 1.0, 300).copy()
kernel = load_model("elliptical_cylinder")
f_sas = DirectModel(empty_data1D(qs), kernel)
sas_pars = dict(scale=1.0, background=0.001,
sld=4.0, sld_solvent=1.0,
radius_minor=20.0, axis_ratio=1.5, length=400.0)
f_sas(**sas_pars)
i1d.device = "gpu"; i1d(qs[:5])
def timeit(fn, n=5):
t0 = time.perf_counter()
for _ in range(n): result = fn()
return (time.perf_counter() - t0) / n * 1e3, result
t_sas, Iq_sas = timeit(lambda: f_sas(**sas_pars))
i1d.device = "gpu"
t_gpu, Iq_gpu = timeit(lambda: i1d(qs), n=3)
i1d.device = "cpu"
t_cpu, Iq_cpu = timeit(lambda: i1d(qs))
i1d.device = "gpu"
print(f"SASView GPU : {t_sas:.0f} ms")
print(f"ESCAPE GPU : {t_gpu:.0f} ms")
print(f"ESCAPE CPU : {t_cpu:.0f} ms ({len(qs)} q-pts)")
rel = np.max(np.abs((Iq_gpu - Iq_sas) / Iq_sas)) * 100
print(f"Max relative diff vs SasView: {rel:.2f}%")
esc.overlay(Iq_sas, Iq_gpu, Iq_cpu, coordinates=qs).config(
xlabel="Q (1/A)", ylabel="I(q) (1/cm)",
xlog=True, ylog=True,
fig_title=f"Elliptical cylinder I(q) — {len(qs)} pts",
labels=["SASView", "ESCAPE GPU", "ESCAPE CPU"],
line_styles=["solid", "dash", "dot"],
line_widths=[2, 3, 3]
)
C:\Users\User\AppData\Local\Temp\ipykernel_49232\923603957.py:16: UserWarning: Input array does not own its data (e.g. it is a view or slice); data will be copied
SASView GPU : 10 ms ESCAPE GPU : 168 ms ESCAPE CPU : 144 ms (300 q-pts) Max relative diff vs SasView: 0.37%