Table 3
Coefficients for H (top) and He (bottom) IS fluxes as parametrised by Eq. (6).
| CR | Coeffs. | MCMC analysis (without Voyager data) | With Voyager | ||||
|
|
|
|
|
|
||
|
|
|||||||
| H | c 0 | 3.6088e+00 | 3.6427e+00 | 3.6753e+00 | 3.5824e+00 | 3.5626e+00 | 3.4617e+00 |
| c 1 | −5.1249e+00 | −5.2323e+00 | −5.3431e+00 | −5.0351e+00 | −4.9695e+00 | −4.1310e+00 | |
| c 2 | −3.1517e+00 | −3.1232e+00 | −3.0871e+00 | −3.1816e+00 | −3.2058e+00 | −4.6403e+00 | |
| c 3 | −1.9668e+00 | −1.8281e+00 | −1.6663e+00 | −2.1007e+00 | −2.1897e+00 | −1.4058e+00 | |
| c 4 | 2.4595e+00 | 2.4752e+00 | 2.4718e+00 | 2.4542e+00 | 2.4545e+00 | −4.7537e+00 | |
| c 5 | 1.8051e+00 | 1.6870e+00 | 1.5352e+00 | 1.9485e+00 | 2.0266e+00 | 8.5077e+00 | |
| c 6 | −5.5338e−01 | −5.6684e−01 | −5.6738e−01 | −5.4072e−01 | −5.3201e−01 | 3.2637e+01 | |
| c 7 | 2.3487e−01 | 2.0121e−01 | 1.6796e−01 | 2.3858e−01 | 2.6123e−01 | −2.8383e+01 | |
| c 8 | −1.2658e+00 | −1.2431e+00 | −1.2024e+00 | −1.2894e+00 | −1.3050e+00 | −5.8203e+01 | |
| c 9 | −2.1496e−01 | −1.9996e−01 | −1.8115e−01 | −2.4841e−01 | −2.5915e−01 | 4.8129e+01 | |
| c 10 | −5.9272e−01 | −5.6908e−01 | −5.4286e−01 | −6.0271e−01 | −6.2241e−01 | 3.3946e+01 | |
| c 11 | 2.9974e−01 | 3.0871e−01 | 3.0692e−01 | 2.9706e−01 | 2.8423e−01 | −2.9586e+01 | |
| c 12 | 6.6289e−01 | 6.5647e−01 | 6.4893e−01 | 6.6907e−01 | 6.7734e−01 | 6.1683e−01 | |
|
−3.7996e+00 | −3.7905e+00 | −3.7836e+00 | −3.8090e+00 | −3.8169e+00 | −3.7995e+00 | |
|
2.7040e+00 | 2.6737e+00 | 2.6415e+00 | 2.7354e+00 | 2.7718e+00 | 2.7040e+00 | |
| He | c 0 | 2.3742e+00 | 2.3953e+00 | 2.4147e+00 | 2.3583e+00 | 2.3461e+00 | 2.2784e+00 |
| c 1 | −5.3456e+00 | −5.4355e+00 | −5.5227e+00 | −5.2749e+00 | −5.2210e+00 | −4.5726e+00 | |
| c 2 | −2.9866e+00 | −2.9022e+00 | −2.8139e+00 | −3.0600e+00 | −3.1233e+00 | −4.8650e+00 | |
| c 3 | −1.3773e+00 | −1.2677e+00 | −1.1418e+00 | −1.4715e+00 | −1.5316e+00 | 3.9567e−01 | |
| c 4 | 2.4858e+00 | 2.3740e+00 | 2.2262e+00 | 2.5976e+00 | 2.6921e+00 | −1.1578e+00 | |
| c 5 | 1.3122e+00 | 1.2090e+00 | 1.0749e+00 | 1.4155e+00 | 1.4734e+00 | 4.9893e+00 | |
| c 6 | −5.5501e−01 | −5.0560e−01 | −4.1371e−01 | −6.2188e−01 | −6.6670e−01 | 1.6511e+01 | |
| c 7 | 1.2550e−01 | 1.1578e−01 | 1.0941e−01 | 1.2485e−01 | 1.2104e−01 | −2.0521e+01 | |
| c 8 | −1.1544e+00 | −1.0715e+00 | −9.6435e−01 | −1.2320e+00 | −1.2943e+00 | −2.8367e+01 | |
| c 9 | −1.7496e−01 | −1.6825e−01 | −1.6336e−01 | −1.8303e−01 | −1.8847e−01 | 3.1850e+01 | |
| c 10 | −5.4768e−01 | −5.2429e−01 | −5.0422e−01 | −5.6130e−01 | −5.7343e−01 | 1.5000e+01 | |
| c 11 | 2.5321e−01 | 2.0779e−01 | 1.4605e−01 | 2.9555e−01 | 3.3392e−01 | −1.7083e+01 | |
| c 12 | 6.6468e−01 | 6.5963e−01 | 6.5218e−01 | 6.7276e−01 | 6.7868e−01 | 6.0486e−01 | |
|
|
−4.9263e+00 | −4.9129e+00 | −4.9009e+00 | −4.9400e+00 | −4.9540e+00 | −4.9261e+00 | |
|
|
2.7141e+00 | 2.6910e+00 | 2.6653e+00 | 2.7448e+00 | 2.7693e+00 | 2.7140e+00 | |
Notes. The parameters c11 and
are combinations of the other parameters. The continuity of the function and its
first derivative at 800
GeV/n
enforces 
and
. The first
five columns correspond to the median and 1 and 2σ CIs of the MCMC
analysis (valid above 400 MeV/n). The last column corresponds to the best-fit fluxes
when accounting for Voyager data (valid to lowest energy Voyager data).
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.