The `MCViNE_LorentzianBroadened_E_Q` Component

Isotropic dispersion E(Q) broadened by a Lorentzian of Q-dependent width.

Identification

Author: Fahima Islam (McStas port of the MCViNE LorentzianBroadened_E_Q_Kernel; MCViNE by J. Y. Y. Lin et al.)
Origin: MCViNE, https://github.com/mcvine/mcvine (mccomponents/lib/kernels/sample/LorentzianBroadened_E_Q_Kernel.icc)
Date: 2026-09-29

Description

S(Q,E) = S(Q) L(E - E(Q); gamma(Q)) with L a Lorentzian of half width at half
maximum gamma(Q).
Q is sampled uniformly in [Qmin,Qmax]; the energy offset is sampled from the
line shape (up to 100 attempts). Neutrons with Ei below min(E(Q)-3w(Q)) do not
scatter.

Functions are given as strings evaluated at run time (MCViNE uses fparser):
+ - * / ^ (or **), % , comparisons, && ||, if(c,a,b), sin cos tan asin acos
atan sinh cosh tanh exp log log10 log2 sqrt abs floor ceil int sign cbrt,
pow atan2 min max hypot fmod, constants pi and e.

Transport (same as MCViNE HomogeneousNeutronScatterer): on the first
passage the neutron is forced to scatter at a uniformly chosen depth, weighted
by path length, attenuation exp(-(mu+sigma)x) and the scattering coefficient;
on exit it is attenuated by exp(-(mu+sigma)L_out). With order>1 further
scatterings are sampled analogically (truncated exponential). With
p_transmit>0 that fraction of events is kept as the attenuated direct beam.
mu(v) = absorption_coefficient*2200/v. Events for which the kernel cannot
scatter (kinematically forbidden) are absorbed.

Geometry: box (xwidth,yheight,zdepth), cylinder (radius,yheight), hollow
cylinder (+thickness) or sphere (radius only). All vectors (Q, targets,
reciprocal vectors, atom positions) are in the component's local frame.

Uses the shared runtime share/mcvine-lib.h/.c.

Example: MCViNE_LorentzianBroadened_E_Q(E_Q="20*sin(Q*1.5)^2", S_Q="1", gamma_Q="0.5", Qmin=0, Qmax=10, scattering_coefficient=10, radius=0.01, yheight=0.05)

Input parameters

Parameters in boldface are required; the others are optional.

Name	Unit	Description	Default
E_Q	str	E(Q) expression [meV], variable Q [AA^-1]	"10"
S_Q	str	S(Q) expression	"1"
gamma_Q	str	Lorentzian HWHM gamma(Q) [meV]	"1"
Qmin	AA^-1	Lower Q bound	0
Qmax	AA^-1	Upper Q bound	10
unbiased	1	0: MCViNE sampling (retries without acceptance correction: over-weights when part of the Q range is forbidden). 1: single attempt, unbiased	0
absorption_coefficient	m^-1	Absorption coefficient at 2200 m/s (MCViNE convention; scales as 1/v)	0
scattering_coefficient	m^-1	Scattering coefficient	0
sigma_abs	barn	Alternative: absorption cross section per unit cell at 2200 m/s (used when Vc>0)	0
sigma_scat	barn	Alternative: scattering cross section per unit cell (used when Vc>0)	0
Vc	AA^3	Unit cell volume; when >0, coefficients are computed from sigma_abs, sigma_scat	0
radius	m	Outer radius of a cylinder (with yheight) or of a sphere (yheight=0)	0
xwidth	m	Width of a box sample	0
yheight	m	Height of a box or cylinder sample	0
zdepth	m	Depth of a box sample	0
thickness	m	Wall thickness of a hollow cylinder (0: filled)	0
pack	1	Packing factor (scales absorption and scattering coefficients)	1
p_transmit	1	Monte Carlo fraction of events kept as unscattered transmitted beam (0: always scatter)	0
order	1	Maximum number of scattering events per neutron (1: single scattering)	1

AT (	,	,		) RELATIVE
ROTATED (	,	,		) RELATIVE

The MCViNE_LorentzianBroadened_E_Q Component

Identification

Description

Input parameters

Links

The `MCViNE_LorentzianBroadened_E_Q` Component