PENELOPE 2003 - OECD Nuclear Energy Agency
PENELOPE 2003 - OECD Nuclear Energy Agency
PENELOPE 2003 - OECD Nuclear Energy Agency
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2.1. Coherent (Rayleigh) scattering 37<br />
where<br />
dσ T (θ)<br />
dΩ<br />
= 1 + cos 2 θ<br />
r2 e<br />
(2.3)<br />
2<br />
is the classical Thomson DCS for scattering by a free electron at rest, θ is the polar<br />
scattering angle (see fig. 2.1) and F (q, Z) is the atomic form factor. The quantity r e is<br />
the classical electron radius and q is the magnitude of the momentum transfer given by<br />
q = 2(E/c) sin(θ/2) = (E/c) [2(1 − cos θ)] 1/2 . (2.4)<br />
In the literature on x-ray crystallography, the dimensionless variable<br />
is normally used instead of q.<br />
x ≡ q 10−8 cm<br />
4π¯h<br />
= 20.6074<br />
q<br />
m e c<br />
(2.5)<br />
The atomic form factor can be expressed as the Fourier transform of the atomic<br />
electron density ρ(r) which, for a spherically symmetrical atom, simplifies to<br />
∫ ∞<br />
F (q, Z) = 4π ρ(r) sin(qr/¯h)<br />
0 qr/¯h r2 dr. (2.6)<br />
F (q, Z) is a monotonically decreasing function of q that varies from F (0, Z) = Z<br />
to F (∞, Z) = 0. The most accurate form factors are those obtained from Hartree-<br />
Fock or configuration-interaction atomic-structure calculations; here we adopt the nonrelativistic<br />
atomic form factors tabulated by Hubbell et al. (1975). Although relativistic<br />
form factors are available (Doyle and Turner, 1968), Hubbell has pointed out that the<br />
non-relativistic form factors yield results in closer agreement with experiment (Cullen<br />
et al., 1997).<br />
where<br />
with<br />
In the calculations, we use the following analytical approximation<br />
⎧<br />
⎪⎨ f(x, Z) ≡ Z 1 + a 1x 2 + a 2 x 3 + a 3 x 4<br />
F (q, Z) =<br />
(1 + a 4 x 2 + a 5 x 4 ) 2 ,<br />
⎪⎩ max {f(x, Z), F K (q, Z)} if Z > 10 and f(x, Z) < 2,<br />
Q =<br />
F K (q, Z) ≡<br />
(2.7)<br />
sin(2b arctan Q)<br />
bQ (1 + Q 2 ) b , (2.8)<br />
q<br />
2m e ca , b = √ 1 − a 2 , a ≡ α(Z − 5/16), (2.9)<br />
where α is the fine-structure constant. The function F K (q, Z) is the contribution to<br />
the atomic form factor due to the two K-shell electrons (see e.g. Baró et al., 1994a).<br />
The parameters of expression f(x, Z) for Z = 1 to 92, which have been determined by<br />
Baró et al. (1994a) by numerically fitting the atomic form factors tabulated by Hubbell<br />
et al. (1975), are included in the block data subprogram PENDAT. The average relative