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Licence: Creative Commons Attribution 4.0 International (CC-BY 4.0) Licence. |
Citatation: Smirnov, Artem; Shprits, Yuri; Allison, Hayley; Aseev, Nikita; Drozdov, Alexander; Kollmann, Peter; Wang, Dedong; Saikin, Anthony (2022): An empirical model of electron pitch angle distributions in the outer radiation belt based on Van Allen Probes data. V. 1.1. GFZ Data Services. https://doi.org/10.5880/GF... |
File format: |
columns 1,2,3 - powers (i,j,k) of the 3D polynomial, see equation (4); |
columns 4,5,6 - c0, c1 and c2 values for the A1 coefficient; |
columns 7,8,9 - c0, c1 and c2 values for the A3 coefficient; |
columns 10,11,12 - c0, c1 and c2 values for the A5 coefficient. |
Note: The model is created for 3.05<L<5.95. For 37 keV channel, it is better to use the model in the outer zone, due to the fact that in the inner zone the shapes are steeper and the fits may not be ideal. |
The polynomials were fitted to degree 7 for the main model. For the high activity bin, the models are fitted to degree 5, because there were less points with Pdyn>5.5 to fit the polynomials and degree 5 was more robust in this case. |
There are two functions to get the PAD coefficients. For values of dynamic pressure below 5.5-6, one should call the "get_coefs" functions, and for the dynamic pressure spikes, one should call the "get_coefs_high" function. |
In case of any questions, contact Artem Smirnov via email: arsmirnov95@gmail.com. |
File format: |
columns 1,2,3 - powers (i,j,k) of the 3D polynomial, see equation (4); |
columns 4,5,6 - c0, c1 and c2 values for the A1 coefficient; |
columns 7,8,9 - c0, c1 and c2 values for the A3 coefficient; |
columns 10,11,12 - c0, c1 and c2 values for the A5 coefficient. |
Note: The model is created for 3.05<L<5.95. For 37 keV channel, it is better to use the model in the outer zone, due to the fact that in the inner zone the shapes are steeper and the fits may not be ideal. |
The polynomials were fitted to degree 7 for the main model. For the high activity bin, the models are fitted to degree 5, because there were less points with Pdyn>5.5 to fit the polynomials and degree 5 was more robust in this case. |
There are two functions to get the PAD coefficients. For values of dynamic pressure below 5.5-6, one should call the "get_coefs" functions, and for the dynamic pressure spikes, one should call the "get_coefs_high" function. |
In case of any questions, contact Artem Smirnov via email: arsmirnov95@gmail.com. |
EL-PASO PAD Model Data
Coefficient files of the empirical electron pitch angle distribution (PAD) model of Smirnov et al. (2022), mirrored from GFZ Data Services for use by EL-PASO. The mirror exists so that EL-PASO can download the coefficients reliably, independent of the availability of the original host.
The files are an unmodified copy of the dataset published at https://doi.org/10.5880/GFZ.2.7.2022.001, restricted to the PAD_model folder plus the accompanying documentation.
Model
The model describes normalized electron PADs in the outer radiation belt, derived from Van Allen Probes data, as a sum of odd sine harmonics:
g(alpha) = A1 * sin(alpha) + A3 * sin(3 * alpha) + A5 * sin(5 * alpha)
Each coefficient A1, A3 and A5 is a 3D polynomial in cos(MLT), sin(MLT) and L, whose terms depend quadratically on the solar wind dynamic pressure Pdyn. See equation (4) of the paper and the model description PDF for details.
- Valid range:
3.05 < L < 5.95. - Energy channels (keV): 37, 56, 78, 106, 142, 179, 220, 246, 342, 453, 588, 735, 871, 1080, 1650.
- For the 37 keV channel, the model is better used in the outer zone, because in the inner zone the shapes are steeper and the fits may not be ideal.
Files
| File | Description |
|---|---|
Pijk_<E>_keV.dat |
Coefficients for energy channel <E> and Pdyn below 5.5 nPa (polynomials of degree 7) |
Pijk_<E>_keV_HIGH.dat |
Coefficients for energy channel <E> during high activity, Pdyn above 5.5 nPa (polynomials of degree 5) |
readme.txt |
Description of the coefficient file format (from the original PAD_model folder) |
read_coefs.py |
Reference implementation for reading and evaluating the coefficients |
2022-001_Smirnov-et-al_readme.txt |
Top-level readme of the original GFZ dataset (license and citation) |
2022-001_Smirnov-et-al_Model-Description.pdf |
Model description |
2022-001_Smirnov-et-al_List-of-files.pdf |
List of files of the original GFZ dataset |
File format
Each Pijk_*.dat file is a plain text table with 12 columns:
| Columns | Content |
|---|---|
| 1, 2, 3 | Powers (i, j, k) of the polynomial term cos(MLT)^i * sin(MLT)^j * L^k |
| 4, 5, 6 | c0, c1, c2 for the A1 coefficient |
| 7, 8, 9 | c0, c1, c2 for the A3 coefficient |
| 10, 11, 12 | c0, c1, c2 for the A5 coefficient |
For each coefficient, the value is c0 * Pdyn^2 + c1 * Pdyn + c2, summed over the polynomial terms in the rows. For Pdyn above 5.5 nPa, use the _HIGH files, in which the coefficients no longer depend on Pdyn.
Usage
from huggingface_hub import hf_hub_download
import numpy as np
path = hf_hub_download(
repo_id="spsw/EL-PASO-PAD-Model-Data",
filename="Pijk_246_keV.dat",
repo_type="dataset",
)
coefs = np.loadtxt(path)
In EL-PASO, the model is available through el_paso.processing.models.get_pa_distribution_smirnov_et_al_2022 and the files are downloaded automatically on first use.
License
The data is licensed under CC BY 4.0, as in the original dataset. Please cite both the data and the paper when using it.
Citation
Data:
Smirnov, Artem; Shprits, Yuri; Allison, Hayley; Aseev, Nikita; Drozdov, Alexander; Kollmann, Peter; Wang, Dedong; Saikin, Anthony (2022): An empirical model of electron pitch angle distributions in the outer radiation belt based on Van Allen Probes data. V. 1.1. GFZ Data Services. https://doi.org/10.5880/GFZ.2.7.2022.001
Paper:
Smirnov et al. (2022), Space Weather. https://doi.org/10.1029/2022SW003053
For questions about the model, the original data contact is Artem Smirnov (arsmirnov95@gmail.com).
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