Bound and Radiation Fields in the Rindler Frame

The energy-momentum tensor of the Liénard-Wiechert field is split into bound and emitted parts in the Rindler frame, by generalizing the reasoning of Teitelboim applied in the inertial frame [see C. Teitelboim, Phys. Rev. D1 (1970), 1572]. Our analysis proceeds by invoking the concept of “energy” defined with respect to the Killing vector field attached to the frame. We obtain the radiation formula in the Rindler frame (the Rindler version of the Larmor formula), and it is found that the radiation power is proportional to the square of acceleration αμ of the charge relative to the Rindler frame. This result leads us to split the Liénard-Wiechert field into a part ĨI, which is linear in αμ, and a part Ĩ, which is independent of αμ. By using these, we split the energy-momentum tensor into two parts. We find that these are properly interpreted as the emitted and bound parts of the tensor in the Rindler frame. In our identification of radiation, a charge radiates neither in the case that the charge is fixed in the Rindler frame, nor in the case that the charge satisfies the equation αμ = 0. We then investigate this equation. We consider four gedanken experiments related to the observer dependence of the concept of radiation.