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High-resolution Interferometric Diagnostics for Ultrashort Pulses

High-resolution Interferometric Diagnostics for Ultrashort Pulses

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Definitions and symbolsAll Fourier trans<strong>for</strong>ms in this dissertation are unitary and use angular frequency. Thesign of the trans<strong>for</strong>m is usually determined by the physical context: a time-to-frequencytrans<strong>for</strong>m has exponential factor e i ωt , whilst a space-to-wavenumber trans<strong>for</strong>m hasexponential factor e −ixk x . In other cases, the sign is explicitly stated. When two quantitiesare related by an integral trans<strong>for</strong>m, such as the Fourier trans<strong>for</strong>m or the Hankeltrans<strong>for</strong>m, they are distinguished by their argument e.g. E (t ) vs E (ω). Specifically, theFourier trans<strong>for</strong>ms of the analytic electric field areE (ω)= 1 2π ∞−∞E (k x )= 1 2π ∞−∞E (t )e i ωt dt E(t )= 1 2π ∞−∞E (x)e −ik x x dx E(x)= 1 2π ∞−∞E (ω)e −itω dωE (k x )e ixk xdk x .The zeroth-order Hankel trans<strong>for</strong>ms are ∞ ∞E (k T )= E (r )J 0 (k T r )r dr E(r )= E (k T )J 0 (k T r )k T dk T .00Several notational conventions are adopted throughout this dissertation. Boldfacesymbols denote vectorial quantities. Where both an italic roman and calligraphic versionof a symbol exist they refer to the analytic (complex-valued) and physical (realvalued)signals respectively. The following table illustrates these two conventions:RealAnalyticScalar EVector E

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