Synchrotron radiation is highly collimated due to the high energy of electrons (over 1 GeV) in strong magnetic fields, resulting in a small opening angle of about 1/2000 radians. The transverse momentum required to produce synchrotron radiation photons is minimal compared to the longitudinal momentum of the electrons. While the Doppler effect influences the observed frequency of the radiation, it does not contribute to the collimation; instead, radiation is emitted in a narrow cone along the electron's velocity vector at relativistic speeds. The beam's size and divergence also depend on factors like the electron beam size, momentum spread, and the bending angle of dipole magnets. Understanding these dynamics can be further explored in texts like "Handbook of Accelerator Physics."