Get Atomic Radiative Processes PDF

By Peter R. Fontana (Auth.)

ISBN-10: 0122620208

ISBN-13: 9780122620201

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It is the interference of a wave train from one path with the same wave train from the other path. The two waves arrive at the detector with a time delay tj — t . 4 Detector Response 35 where we set Uj = Γ ^ . The response of the detector is given by the sum of the energies of the wave trains plus a set of interference terms determined by the mutual coherence functions. F r o m Eq. 66) / / ω ) / * ( ω ) 6 χ ρ [ ί ω ( ί - i )] dco 7 fc The steps in Eq. 66) are the same as the ones in Eqs. 20). 67) which for 7 = fc agrees with Eq.

Coherence Properties of Waves In addition, the Doppler effect shifts the central frequency of the wave. The detector thus receives pulses with different frequencies and durations. We assume that we have an ideal square law detector with a broad enough frequency response so as not to modify the pulse shape. W e first analyze the response of the detector after one pulse has been received. 4 we consider the response due to several wave trains. 1 Spectrum of a Sinusoidal Pulse of Constant Amplitude The wave train has a frequency ω and duration T.

28 2. Coherence Properties of Waves In addition, the Doppler effect shifts the central frequency of the wave. The detector thus receives pulses with different frequencies and durations. We assume that we have an ideal square law detector with a broad enough frequency response so as not to modify the pulse shape. W e first analyze the response of the detector after one pulse has been received. 4 we consider the response due to several wave trains. 1 Spectrum of a Sinusoidal Pulse of Constant Amplitude The wave train has a frequency ω and duration T.

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Atomic Radiative Processes by Peter R. Fontana (Auth.)


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