erlab.analysis.fit.functions.general¶
Some general functions and utilities used in fitting.
Many functions are numba
-compiled for speed.
Module Attributes
From |
Functions
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Interpolation formula for a temperature dependent BCS-like gap. |
|
Convolves |
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Dynes formula for superconducting density of states. |
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Fermi-dirac edge in terms of temperature. |
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Fermi-dirac edge with linear backgrounds above and below the fermi level. |
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Resolution-broadened Fermi edge with linear backgrounds above and below EF. |
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Gaussian parametrized with FWHM and peak height. |
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Lorentzian parametrized with FWHM and peak height. |
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Step function convolved with a Gaussian. |
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Resolution broadened step function with linear backgrounds. |
- erlab.analysis.fit.functions.general.bcs_gap(x, a=1.76, b=1.74, tc=100.0)[source]¶
Interpolation formula for a temperature dependent BCS-like gap.
\[\Delta(T) \simeq a \cdot k_B T_c \cdot \tanh\left(b \sqrt{\frac{T_c}{T} - 1}\right)\]- Parameters:
x (
array-like
) – The temperature values in kelvins at which to calculate the BCS gap.a (float) – Proportionality constant. Default is 1.76.
b (float) – Proportionality constant. Default is 1.74.
tc (float) – The critical temperature in Kelvins. Default is 100.0.
- erlab.analysis.fit.functions.general.do_convolve(x, func, resolution, pad=5, **kwargs)[source]¶
Convolves
func
with gaussian of FWHMresolution
inx
.- Parameters:
x (ndarray[Any, dtype[float64]]) – A evenly spaced array specifing where to evaluate the convolution.
func (Callable) – Function to convolve.
resolution (float) – FWHM of the gaussian kernel.
pad (int) – Multiples of the standard deviation \(\sigma\) to pad with.
**kwargs – Additional keyword arguments to
func
.
- erlab.analysis.fit.functions.general.do_convolve_2d(x, y, func, resolution, pad=5, **kwargs)[source]¶
- erlab.analysis.fit.functions.general.dynes(x, n0=1.0, gamma=0.003, delta=0.01)[source]¶
Dynes formula for superconducting density of states.
The formula is given by [4]:
\[f(x) = N_0 \text{Re}\left[\frac{|x| + i \Gamma}{\sqrt{(|x| + i \Gamma)^2 - \Delta^2}}\right]\]where \(x\) is the binding energy, \(N_0\) is the normal-state density of states at the Fermi level, \(\Gamma\) is the broadening term, and \(\Delta\) is the superconducting energy gap.
- Parameters:
x (
array-like
) – The input array of energy in eV.n0 – \(N_0\), by default 1.0.
gamma – \(\Gamma\), by default 0.003.
delta – The superconducting energy gap \(\Delta\), by default 0.01.
- erlab.analysis.fit.functions.general.fermi_dirac(x, center, temp)[source]¶
Fermi-dirac edge in terms of temperature.
- erlab.analysis.fit.functions.general.fermi_dirac_linbkg(x, center, temp, back0, back1, dos0, dos1)[source]¶
Fermi-dirac edge with linear backgrounds above and below the fermi level.
Note
back0
andback1
corresponds to the linear background above and below EF (due to non-homogeneous detector efficiency or residual intensity on the phosphor screen during sweep mode), whiledos0
anddos1
corresponds to the linear density of states below EF including the linear background.
- erlab.analysis.fit.functions.general.fermi_dirac_linbkg_broad(x, center, temp, resolution, back0, back1, dos0, dos1)[source]¶
Resolution-broadened Fermi edge with linear backgrounds above and below EF.
- erlab.analysis.fit.functions.general.gaussian_wh(x, center, width, height)[source]¶
Gaussian parametrized with FWHM and peak height.
Note
\(\sigma=\frac{w}{2\sqrt{2\log{2}}}\)
- erlab.analysis.fit.functions.general.lorentzian_wh(x, center, width, height)[source]¶
Lorentzian parametrized with FWHM and peak height.
Note
\(\sigma=w/2\)
- erlab.analysis.fit.functions.general.step_broad(x, center=0.0, sigma=1.0, amplitude=1.0)[source]¶
Step function convolved with a Gaussian.