Table 1.
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Boundaries of the uniform priors on the model parameters. The lower bound on |${\mathcal {R}}_l$| is chosen to be smaller than the rigidity at which the diffusion time-scale becomes smaller than the advection and energy loss time-scales.

α|$\kappa _{\mathrm{halo}}\, [\mathrm{pc^2\,yr^{-1}}]$||$H\, [\mathrm{kpc}]$||$v_c\, [\mathrm{km\,s^{-1}}]$|δδl|${\mathcal {R}}_l\, [\mathrm{GV}]$|
[0, 1][0.001, 1][0.1, 20][0.01, 100][0, 2][−4, 4][2.2, 20]
α|$\kappa _{\mathrm{halo}}\, [\mathrm{pc^2\,yr^{-1}}]$||$H\, [\mathrm{kpc}]$||$v_c\, [\mathrm{km\,s^{-1}}]$|δδl|${\mathcal {R}}_l\, [\mathrm{GV}]$|
[0, 1][0.001, 1][0.1, 20][0.01, 100][0, 2][−4, 4][2.2, 20]
Table 1.
Open in new tab

Boundaries of the uniform priors on the model parameters. The lower bound on |${\mathcal {R}}_l$| is chosen to be smaller than the rigidity at which the diffusion time-scale becomes smaller than the advection and energy loss time-scales.

α|$\kappa _{\mathrm{halo}}\, [\mathrm{pc^2\,yr^{-1}}]$||$H\, [\mathrm{kpc}]$||$v_c\, [\mathrm{km\,s^{-1}}]$|δδl|${\mathcal {R}}_l\, [\mathrm{GV}]$|
[0, 1][0.001, 1][0.1, 20][0.01, 100][0, 2][−4, 4][2.2, 20]
α|$\kappa _{\mathrm{halo}}\, [\mathrm{pc^2\,yr^{-1}}]$||$H\, [\mathrm{kpc}]$||$v_c\, [\mathrm{km\,s^{-1}}]$|δδl|${\mathcal {R}}_l\, [\mathrm{GV}]$|
[0, 1][0.001, 1][0.1, 20][0.01, 100][0, 2][−4, 4][2.2, 20]
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