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Engineering LibreTexts

1.2: Pulse Characteristics

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Most often, there is not an isolated pulse, but rather a pulse train.

截屏2021-03-24 下午7.24.41.png
Figure 1.1: Periodic 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 ns30 cm (high-speed electronics, GHz1 ps300 μm1 fs300 nm1 as=1018s0.3 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!

截屏2021-03-24 下午7.41.37.png
Figure 1.2: Electric field waveform of a 5 fs pulse at a center wavelength of 800 nm. The electric field depends on the carrier-envelope phase.

average power:

Pave1W, up to 100 W in progress. kW possible, not yet pulsed

repetition rates:

T1R=fR=m Hz - 100 GHz

pulse energy:

W=1pJ1kJ

pulse width:

τFWHM=5 fs - 50 ps,modelocked30 ps - 100 ns,Q - switched

peak power:

Pp=1 kJ1 ps1 PW,

obtained with Nd:glass (LLNL - USA, [1][2][3]).

For a typical lab pulse, the peak power is

Pp=10 nJ10 fs1 MW

peak field of typical lab pulse:

Ep=2×377×106×1012π×(1.5)2Vm1010Vm=10Vnm


This page titled 1.2: Pulse Characteristics is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Franz X. Kaertner (MIT OpenCourseWare) via source content that was edited to the style and standards of the LibreTexts platform.

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