Femtosecond pulse shaping

In optics, femtosecond pulse shaping refers to manipulations with temporal profile of an ultrashort laser pulse. Pulse shaping can be used to shorten/elongate the duration of optical pulse, or to generate complex pulses.

Introduction

Fig. 1: Schematic diagram of a Pulse Shaper

Generation of sequences of ultrashort optical pulses is key in realizing ultra high speed optical networks, Optical Code Division Multiple Access (OCDMA) systems, chemical and biological reaction triggering and monitoring etc. Based on the requirement, pulse shapers may be designed to stretch, compress or produce a train of pulses from a single input pulse. The ability to produce trains of pulses with femtosecond or picosecond separation implies transmission of optical information at very high speeds.

In ultrafast laser science pulse shapers are often used as a compliment to pulse compressors in order to fine-tune high-order dispersion compensation and achieve transform-limited few-cycle optical pulses.^[1]

Techniques

A pulse shaper may be visualized as a modulator. The input pulse is multiplied with a modulating function to get a desired output pulse. The modulating function in pulse shapers may be in time domain or a frequency domain (obtained by Fourier Transform of time profile of pulse). However, application of direct pulse shaping technique on a femtosecond time scale faces the same problem as direct femtosecond pulse measurement: electronics speed limitations.^[2] Michelson interferometer can be regarded as direct space-to-time pulse shaper since position of the moving mirror is directly transferred to the inter-pulse delay of the output pulse pair.

Fourier transform pulse shaping

An ultrashort pulse with a well-defined electrical field $E(t)$ can be modified with an appropriate filter acting in the frequency domain. Mathematically, the pulse is Fourier transformed, filtered, and back-transformed to yield a new pulse:

E'(t) = \mathcal{F}^{-1}\{\mathcal{F}\{E(t)\}(\omega)f(\omega)\}(t).

It is possible to design an optical setup with an arbitrary filter function $f(\omega)$ which can be complex-valued, as long as $|f(\omega)|\le1$ . Figure 1 shows how a bandwidth-limited pulse could be transformed into a chirped pulse (with a filter only acting on the phase) or into a more complex pulse (with the filter acting on both phase and amplitude).

Design

One can distinguish FT pulse shapers by their optical design: i.e., collinear shapers and transverse shapers, and by their programmability, i.e., static (or manually adjustable) shapers and programmable shapers.^[3]

Examples

Collinear static: propagation in dispersive medium, chirped mirror
Collinear programmable: AOPDF

Transverse static: pulse stretcher/compressor (static mask in Fourier plane can be added for amplitude shaping)
Transverse programmable: spatial light modulator inserted in a zero-dispersion line ^[4]

Notes

↑ Hagemann, Franz; Oliver Gause; Ludger Wöste; Torsten Siebert (2013-03-11). "Supercontinuum pulse shaping in the few-cycle regime". Optics Express 21 (5): 5536–5549. Bibcode:2013OExpr..21.5536H. doi:10.1364/OE.21.005536. Retrieved 2013-06-11.
↑ Diels, Jean-Claude; Wolfgang Rudolph (2006). "Pulse Shaping". Ultrashort Laser Pulse Phenomena. Burlington: Academic Press. pp. 433–456. ISBN 978-0-12-215493-5.
↑ Monmayrant, Antoine; Sébastien Weber; Béatrice Chatel (2010-05-28). "A newcomer's guide to ultrashort pulse shaping and characterization". Journal of Physics B: Atomic, Molecular and Optical Physics 43 (10): 103001. Bibcode:2010JPhB...43j3001M. doi:10.1088/0953-4075/43/10/103001. ISSN 0953-4075. Retrieved 2013-06-11.
↑ A.M. Weiner. "Femtosecond pulse shaping using spatial light modulators". Review of Scientific Instruments 71 , 1929-1960 (2000).