Expand description
Oen-Robinson local (impact-parameter dependent) electronic energy loss.
O. S. Oen and M. T. Robinson, Nucl. Instrum. Methods 132, 647 (1976).
The nonlocal part is Lindhard-Scharff with the same k_L. The local model
assigns a collision with closest approach r_min the loss
ΔE_e(E, r_min) = S_LS(E) · c² / (2π a²) · exp(-c r_min / a), c = 0.3,
with a the Firsov screening length 0.8853 a0 (Z1^(1/2) + Z2^(1/2))^(-2/3).
The prefactor normalises ∫ ΔE_e 2π p dp = S_LS when r_min is identified
with the impact parameter p; that identification is the approximation made
in the original paper, so the impact-averaged stopping equals the LS value.
The constants c = 0.3 and the choice of length were entered from the
literature as remembered by the contributor and have not been verified
against the 1976 paper; see docs/data-provenance.md and
OR_CONSTANTS_UNVERIFIED. A secondary source, J. F. Ziegler,
J. P. Biersack, M. D. Ziegler, SRIM: The Stopping and Range of Ions in
Matter (SRIM Co., 2015), Eq. 7-45, p. 7-17, prints
ΔE = 0.045 k √E / (π a²) exp(-0.3 r0 / a), which confirms c = 0.3 and
the prefactor c² / (2π), but not which screening length a is.
Structs§
- OenRobinson
- Oen-Robinson model.
stoppingis the impact-averaged value; useOenRobinson::local_lossfor the per-collision loss.
Constants§
- OR_
CONSTANTS_ UNVERIFIED - Whether the constants of the local model (
OR_EXPONENT_COEFFICIENTand the length oflocal_length) are still not verified against Oen and Robinson, Nucl. Instrum. Methods 132, 647 (1976).truewhile the Oen-Robinson row ofdocs/data-provenance.mdsays “not verified”. - OR_
EXPONENT_ COEFFICIENT - Exponent coefficient
cinexp(-c r_min / a).
Functions§
- local_
length - Firsov-type screening length used by the local model, m.