BIOPHOTONICS: Optical protein switches at picosecond speeds

The development of all-optical data processing is getting a boost from European researchers who are pioneering the use of an optically active protein for ultrafast photonic switching.

Oct 1st, 2011
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The development of all-optical data processing is getting a boost from European researchers who are pioneering the use of an optically active protein for ultrafast photonic switching.1 Their technique could one day achieve switching speeds faster than 1 Tbit/s.

The group, from the Biological Research Centre of the Hungarian Academy of Sciences, the HAS Research Group of Laser Physics, and the University of Szeged (all in Szeged, Hungary) and the University of Witten/Herdecke (Witten, Germany) has based its experiment on bacteriorhodopsin (bR), which has numerous illumination-driven transitions to quasi-stable states, two of which are ultrafast.

Fast intermediate state

Bacteriorhodopsin is a purple bacterial chromoprotein that, unlike many proteins, is physically robust. When subjected to light, it pumps protons through its membrane via numerous sequential intermediate states with different switching speeds and all of which change the refractive index and absorption. These states can be switched back to the ground state via a second light pulse.

Switching speeds range from sub-picosecond to a few tenths of a second. The researchers chose the “BR→K” picosecond-rate transition.

A bR layer was deposited on top of a titanium dioxide singlemode thin-film waveguide that contains a 2400 lines/mm coupler grating between it and the glass substrate. This became the central piece in a pump-probe experiment using picosecond and femtosecond pulses. With a 530 nm wavelength, the pump pulse lies within the absorption band of bR, while the 790 nm probe pulse has a wavelength that is not absorbed by any of the intermediate transitions.

A pump pulse changes the refractive index of a bR sample; as a result, the wavelength of a portion of a probe pulse selected by a grating changes at picosecond speed.

The pump and probe light was obtained from a terawatt laser, with the 530 nm pulses arising from a combination of noncollinear optical parametric chirped-pulse amplification and chirp-assisted sum-frequency generation and the 790 nm pulses coming directly from the beam. After spectral shaping, the pulses were aimed at the sample, arriving at different times as required for the pump-probe technique.

Two sets of experiments were carried out. The first relied on non-transform-limited pump-pulse durations between 3.2 and 12 ps and a 100 ps delay. Here, the excitation of the bR caused the wavelength of the light incoupled by the grating to be shifted toward the red, producing what the researchers called “frequency switching.” In a practical device, this effect, caused by a fast change in the refractive index, would allow different bands of sub-nanometer linewidth to be selected from a broadband pulse, allowing frequency demultiplexing.

The second set of experiments explored using the fastest bR transition, the “BR→I” transition. Transform-limited pump pulses with durations of 150 fs were used. Two situations were tested: pump and probe pulses with no time delay, and a probe without the pump (excitation) pulses. Here, the intensity of the probe was diminished when the pump was added, showing a potential path to sub-femtosecond switching. —John Wallace

REFERENCE
1. L. Fábián et al., Opt. Exp., 19, 20, 18861 (Sept. 26, 2011).

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