Bound states in the continuum (BIC) microlasers reach ultrafast switching speeds

April 14, 2020
By creating a high-quality cavity without the typical physical confinement, BIC microlasers with highly directional output and single-mode operation are breaking the tradeoff between energy consumption and switching speed.
(Image credit: Harbin University)
In the two-beam pumping experiment (a), two beams are spatially detuned with a distance d < 2R, being shifted temporally with a delay time τ. The insets show the far-field emission patterns from the perovskite metasurface under both symmetric and asymmetric excitations. In the transition from a BIC microlaser to a linearly polarized (LP) laser (b), I1,2 are the intensities at the marked regions in the inset to (a). Insets show the corresponding beam profiles. The reverse transition is also shown from LP to BIC microlaser (c). Finally, the transition from a donut beam to a two-lobe beam and back within a few picoseconds is shown (d); red curves are guiding lines for the calculation of the transition time.
In the two-beam pumping experiment (a), two beams are spatially detuned with a distance d < 2R, being shifted temporally with a delay time τ. The insets show the far-field emission patterns from the perovskite metasurface under both symmetric and asymmetric excitations. In the transition from a BIC microlaser to a linearly polarized (LP) laser (b), I1,2 are the intensities at the marked regions in the inset to (a). Insets show the corresponding beam profiles. The reverse transition is also shown from LP to BIC microlaser (c). Finally, the transition from a donut beam to a two-lobe beam and back within a few picoseconds is shown (d); red curves are guiding lines for the calculation of the transition time.

Scientists at Harbin Institute of Technology (Harbin, China), Australian National University (Canberra, ACT, Australia), and City University of New York (New York, NY) have applied the concept of bound states in the continuum (BIC) to microlasers, breaking the long-standing tradeoff between ultralow energy consumption and ultrafast switching.1

In past decades, requirements for all-optical switches have included low energy consumption, high speed, strong modulation ratio, small footprint, and on-chip integration. The small footprint and on-chip integration are quite easy for current nanotechnologies—however, the tradeoff between low energy consumption and high speed is a severe challenge. The conventional approach focuses on enhancing the light-matter interaction via on-chip integrated micro- or nanocavities. But while the relatively high Q factor of a resonator can effectively increase the local electromagnetic response, the corresponding increase in mode lifetime with increase in Q also restricts the response of the switch. And unfortunately, other methods with ultrasmall effective mode volume such as plasmonic nanostructures are limited by large coupling and propagation loss.

Bound states in the continuum

By focusing on laser emission from topologically protected BIC microlasers, the power/switching tradeoff can be addressed. Owing to the far-field characteristics of BIC lasers, the transition from BIC microlasers to conventional lasers represents a redistribution of the laser emission instead of direct on/off switching of the lasing mode. This means the switching process is not limited by the lifetime of the resonant mode.

Because the BICs can eventually have infinitely large Q factors, the laser thresholds can be reduced by orders of magnitude, making it possible to realize the ultrafast optical switching that match all the requirements of modern classic and quantum information.

In square-latticed MAPbBr3 perovskite periodic nanostructures, the researchers have realized single-mode laser emission with donut beam profiles. As expected, they have confirmed the relationship between the symmetry of the pumping profile and the emission beam profile. By applying the second beam with spatial and temporal deviation, the four-fold rotational symmetry of the square lattice is broken in a very short time and the BIC laser degrades to a conventional photonic-crystal laser with two linearly polarized lobes.

The transition process takes place in 1 to 1.5 ps; complete transition from a donut to two lobes and back to a donut has also been realized within 2 to 3 ps. Such switching times are more than an order of magnitude faster than the BIC microlaser lifetime, clearly demonstrating that the limitation of laser lifetime on the switching time is broken.

Presently, the team is working on the reduction of energy consumption and cascaded on-chip integration of the ultrafast switchable BIC lasersa key step towards efficient optical and quantum computing.

REFERENCE

1. C. Huang et al., Science, 367, 10181021 (2020).

About the Author

Gail Overton | Senior Editor (2004-2020)

Gail has more than 30 years of engineering, marketing, product management, and editorial experience in the photonics and optical communications industry. Before joining the staff at Laser Focus World in 2004, she held many product management and product marketing roles in the fiber-optics industry, most notably at Hughes (El Segundo, CA), GTE Labs (Waltham, MA), Corning (Corning, NY), Photon Kinetics (Beaverton, OR), and Newport Corporation (Irvine, CA). During her marketing career, Gail published articles in WDM Solutions and Sensors magazine and traveled internationally to conduct product and sales training. Gail received her BS degree in physics, with an emphasis in optics, from San Diego State University in San Diego, CA in May 1986.

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