The polarization emerging in the subsequent scattering processes can never exceed 1 which corresponds to the fully polarized pure state. This property is shown to be provided by the addition rule similar to that for relativistic velocities never exceeding the speed of light. The cases of spin ${\displaystyle 1/2}$ and 1 are considered. The photon linear polarization in subsequent Thomson scattering processes is monotonically increasing. This directness is shown to be a consequence of spin measurement procedure and may be the particular example of the anticipated relation between quantum measurement and time irreversibility. The emergent polarization may be considered as a case of the opposing time's arrows corresponding to microscopic (spin) and macroscopic (momentum) degrees of freedom, respectively.

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• Polarization
• Spin