StaticLorentzianKT¶

Description¶

Static Lorentzian Kubo-Toyabe function:

$g_{z}^{L}(t,B_L) = A_0 \{1 - \frac{a}{\omega_{L}}j_1(\omega_{L}t)e^{-at}-\left(\frac{a}{\omega_L}\right)^2(j_o(\omega_{L}t)e^{-at}-1)-\left(1+\left(\frac{a}{\omega_L}\right)^2\right)a\int_{0}^{t}j_0(\omega_{L}\tau)e^{-a\tau}d\tau\}$

where,

$L$ refers to Lorentzian,

$B_L$ refers to the longitudinal field applied to the z-axis,

$j_{i}$ are the spheical Bessel functions of the First Kind,

$\omega_L$ is is the precessing angular frequency and its relationship is given by $B_L= \omega_{L} / \gamma_{\mu}$ ,

$\gamma_{\mu}$ is the gyromagnetic ratio of muons,

and $a (\mu s^{-1})$ is the half-width at half maximum of the Lorentzian distribution.

(Source code, png, hires.png, pdf)

Properties (fitting parameters)¶

Name	Default	Description
A0	0.2
A	0.1	Half-width of half maximum of Lorentzian distribution (microsecs)
Field	0.1	Longitudinal B-field (G)

References¶

[1] Y. Uemura et al., Phys. Rev. B 31 546 (1985).

Categories: FitFunctions | MuonGeneric

Source¶

Python: StaticLorentzianKT.py (last modified: 2019-11-14)