1.2: Pulse Characteristics
( \newcommand{\kernel}{\mathrm{null}\,}\)
Most often, there is not an isolated pulse, but rather a pulse train.

TR: pulse repetition time
W : pulse energy
Pave=W/TR: average power
τFWHM is the Full Width at Half Maximum of the intensity envelope of the pulse in the time domain.
The peak power is given by
Pp=WτFWHM=PaveTRτFWHM
and the peak electric field is given by
\[E_p = \sqrt{2 Z_{F_0} \dfrac{P_p}{A_{\text{eff}}} \nonumber \]
Aeff is the beam cross-section and ZF0=377Ω is the free space impedance.
Time scales:
1 ns∼30 cm (high-speed electronics, GHz1 ps∼300 μm1 fs∼300 nm1 as=10−18s∼0.3 nm = 3A˚
The shortest pulses generated to date are about 4 - 5 fs at 800 nm (\lambda/c = 2.7 fs), less than two optical cycles and 250 as at 25 nm. For few-cycle pulses, the electric field becomes important, not only the intensity!

average power:
\begin{array} {cl} {P_{ave} \sim} & {\text{1W, up to 100 W in progress.}} \\ {\ } & {\text{kW possible, not yet pulsed}} \end{array} \nonumber
repetition rates:
T_R^{-1} = f_R = \text{m Hz - 100 GHz}\nonumber
pulse energy:
W = 1pJ - 1kJ\nonumber
pulse width:
\tau_{\text{FWHM}} = \begin{array} {ll} {\text{5 fs - 50 ps,}} & {\text{modelocked}} \\ {\text{30 ps - 100 ns,}} & {\text{Q - switched}} \end{array}\nonumber
peak power:
P_p = \dfrac{\text{1 kJ}}{\text{1 ps}} \sim \text{1 PW},\nonumber
obtained with Nd:glass (LLNL - USA, [1][2][3]).
For a typical lab pulse, the peak power is
P_p = \dfrac{\text{10 nJ}}{\text{10 fs}} \sim \text{1 MW}\nonumber
peak field of typical lab pulse:
E_p = \sqrt{2 \times 377 \times \dfrac{10^6 \times 10^{12}}{\pi \times (1.5)^2}} \dfrac{\text{V}}{\text{m}} \approx 10^{10} \dfrac{\text{V}}{\text{m}} = \dfrac{10\text{V}}{\text{nm}}\nonumber