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Figure S6.

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y, proton flux observations (normalized to the equatorial flux intensity of the shell), as a function of x=(Hmin-50)/(Hmin,eq(L)-50) $ x=({H}_{{min}}-50)/({H}_{{min},{eq}}(L)-50)\enspace $in four L shells. Discrete data points: based on observations within the L-shell interval by RPS-b in year 2013 (red: >192 MeV; green: >300 MeV); Solid line: gh function for the shell (see Equation (8), with the value of η indicated; Vertical dashed line: Hmin( B/B0)$ {H}_{{min}}\left(\enspace {B}/{B}_0\right)$ = 1000 km, separating the high-altitude region and the low-altitude region of the environment.

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