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Optics Fourier Transform Ii
Lecture03 Ultrashort Pulses 01 (1)
z n + a n-1 z +... +a 0 = (z – z n ) (z – z n-1 )... (z – z 1 ) and the Measurement of the Shortest Rick Trebino School of Physics Georgia Institute of.
Ultrashort Laser Pulses I Description of pulses Intensity and phase The instantaneous frequency and group delay Zero th and first-order phase The linearly.
The dilemma The goal: measuring the intensity and phase vs. time (or frequency) Why? The Spectrometer and Michelson Interferometer 1D Phase Retrieval.