A charge moving uniformly through a transparent dielectric can emit Cherenkov radiation if its speed exceeds the phase velocity of light in that medium:
It need not exceed the vacuum speed . The passing charge polarizes the medium; the induced response produces radiation that adds coherently along selected directions. Equivalently, phase matching along the trajectory requires . Since ,
Here is the angle of the emitted light rays to the forward particle velocity: the rays form a cone around the track. With dispersion, both the threshold and cone angle depend on frequency; only transparent frequency bands satisfying the threshold contribute escaping radiation.
In the wavefront construction, a disturbance emitted a time earlier has radius , while the particle has moved . Tangents from the present particle position to these wavefronts make a backward-opening wavefront cone of half-angle , where . The light rays are normal to this cone. Consequently : the Cherenkov photon-cone and wavefront-cone angles are complementary, rather than identical.
First obtain the particle speed from kinetic energy rather than treating as its total energy. With Electron rest energy ,
For Cherenkov radiation, the photon propagation direction makes angle to the particle trajectory, with . The speed correction is negligible at three significant digits, but the Cherenkov photon-cone and wavefront-cone angles must be distinguished.
If the given opening is the full cone of photon directions, . The result is
If instead denotes the full opening of the conical wavefront, its half-angle is complementary to the photon direction: . That convention gives
The original PDF supplies no cone diagram or definition distinguishing these geometries. Thus the literal full photon-cone interpretation gives , while follows from the wavefront interpretation. It would be incorrect to interchange sine and cosine without stating which cone is meant.
Figure 1.
Photon-direction and wavefront cone openings are complementary geometries, giving different interpretations of the supplied angle
. Details.