Line widths in the fast-motional regime.
lw = fastmotion(Sys,B0,tcorr) lw = fastmotion(Sys,B0,tcorr,domain) [lw,mI] = fastmotion(...)
Given the g, A and Q tensors in Sys
, the magnetic field (mT) in B0
and a rotation correlation time (seconds) in tcorr
, fastmotion
computes the EPR line widths resulting from rotational motion of the paramagnetic molecules. The widths depends on the anisotropies of g, A and Q. The widths are returned in lw
(in units of mT or MHz, depending on domain
), and the associated lines are identified by sets of mI numbers in mI
. One row corresponds to one EPR resonance line.
The four input parameters are
Sys
Nucs
, the g, A and Q tensors g
, A
, Q
, and, optionally, the tensor orientations in gFrame
and AFrame
. The field QFrame
is not used.B0
tcorr
tcorr
and the diffusion rate D
are related by tcorr = 1/(6*D)
.domain
'field'
for field sweeps (units of mT) or 'freq'
for frequency sweeps (units MHz). Default is 'field'
.
The two output parameters are
lw
mI
fastmotion
uses the Kivelson formula to compute line widths.
Outside the fast-motion regime (Redfield limit, motional narrowing),
the formulas are not valid.
The formulas used in fastmotion
are from Neil Atherton, Principles
of Electron Spin Resonance, 1993. The relevant expressions are on pages 331
(9.2.48-51) and 348 (9.5.2).
The original theory can be found in J.H. Freed and G.K. Fraenkel, J. Chem. Phys. 39 (1963), 326-348.
The X-band spectrum of a nitroxide radical in the fast motional regime features three lines with different widths. The widths and the mI values for the associated lines are
Nitroxide = struct('g',[2.0088 2.0064 2.0027],'Nucs','14N'); Nitroxide.A = unitconvert([7.59 5.95 31.76]/10,'mT->MHz'); Field = 350; tcorr = 1e-10; [lw,mI] = fastmotion(Nitroxide,Field,tcorr,'field')
lw = 0.0070 0.0029 0.0027 mI = -1 0 1