1.2: Pulse Characteristics
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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 = 3˚A (typ-lattice constant in metal)
The shortest pulses generated to date are about 4 - 5 fs at 800 nm (λ/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:
Pave∼1W, up to 100 W in progress. kW possible, not yet pulsed
repetition rates:
T−1R=fR=m Hz - 100 GHz
pulse energy:
W=1pJ−1kJ
pulse width:
τFWHM=5 fs - 50 ps,modelocked30 ps - 100 ns,Q - switched
peak power:
Pp=1 kJ1 ps∼1 PW,
obtained with Nd:glass (LLNL - USA, [1][2][3]).
For a typical lab pulse, the peak power is
Pp=10 nJ10 fs∼1 MW
peak field of typical lab pulse:
Ep=√2×377×106×1012π×(1.5)2Vm≈1010Vm=10Vnm