Kierkegaard as Phenomenologist
DOI: 10.2307/j.ctv47w62p.9
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“…(33) for w when T ∈ [T n−1 , T n−1/2 ], where the time intervals can be approximated by Eqs. (34) and (35). The oscillation half period in the lab frame is then…”
Section: Experimental Signatures: Chirping Of Radiationmentioning
confidence: 99%
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“…(33) for w when T ∈ [T n−1 , T n−1/2 ], where the time intervals can be approximated by Eqs. (34) and (35). The oscillation half period in the lab frame is then…”
Section: Experimental Signatures: Chirping Of Radiationmentioning
confidence: 99%
“…As the particle decelerates from the speed of light, its radiation power is a constant. The radiation energy increases linearly, while the Schott energy decreases linearly at exactly the same rate such that the sum of the radiation energy and the Schott energy is a constant [35]. In this way, the decrease of the Schott energy completely accounts for the increase of the radiation energy, and the charged particle radiates without losing any of its mechanical energy.…”
Section: Introductionmentioning
confidence: 96%