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High Chern Numbers in Photonic Crystals

High Chern Numbers in Photonic Crystals topological concepts to describe condensed-matter systems was first put forward in the description of the integer quantum Hall effect by David Thouless, Mahito Kohmoto, Peter Nightingale, and Marcel den Nijs [4]. They showed that the Hall conductance of a two-dimensional electron system under a large magnetic field can be quantized, that is, fixed to be an integer times a fundamental constant, e2 /h. That integer, DOI: 10.1103/Physics.8.122 URL: http://link.aps.org/doi/10.1103/Physics.8.122 known as the Chern number, corresponds to the number of edge states that carry current, without scattering, across the system. The Chern number indicates topological behavior in the sense that small deformations of the system (such as disorder, strain, and localized defects) have little effect on its properties. This makes the system’s physics independent of its minute details (such as hopping parameters, number of dopants, or atomic constituents) and only dependent on this global quantity, which must be an integer. In other words, it depends on the system’s topology rather than on its geometry. Although the initial interest in topological phenomena focused on electrons, topological behavior can be generalized to any type of wave, including light, as first predicted in Ref. [5]. A magnetic photonic crystal—a photonic crystal made of materials that break Lorentz reciprocity due to their response to an external magnetic field—can have a nonzero Chern number (and associated nonscattering edge states) for electromagnetic modes, that is, photons, rather than electrons. Soljačić’s group demonstrated this in 2009, showing that a topological protection of microwave photons could be observed in photonic crystals [6]. The finding launched a search for the realization of topological insulators for photons at optical wavelengths [7], motivated by the prospect of engineering robust optical devices, immune to disorder. Using similar mechanisms as in Ref. [6] proved challenging because of the weakness of magnetic effects in the optical regime. But alternative mechanisms later enabled robust topological edge states for light in a photonic lattice [8] and silicon ring resonator arrays [9]. Employing a microwave photonic crystal similar to the one they used previously [6], Soljačić’s team now reports another important discovery, that of high-Chern number (> 1) bands in a photonic quantum anomalous Hall system. The authors utilized a scheme (see Fig. 1) based on two-dimensional photonic crystals made of ferromagnetic garnet rods sandwiched between two copper plates. Simc 2015 American Physical Society tromagnetic field transmitted by the crystal. (An advantage of the microwave regime is that phase information is much easier to collect than in optics.) By Fourier transforming the spatial profile of the edge states, they determined their lattice momentum as a function of frequency, mapping out their band structure and determining the Chern numbers of each band. As a result of the higher-Chern-number bands, there are multiple edge states that cross the band gaps of the photonic crystal [2]. To my knowledge, the data collected by Soljačić’s team are the first direct experimental characterization of the band structure of a one-dimensional topological edge state. This work demonstrates the surprising generality of topological physics and the fact that alternative wavebased systems, such as photonics, can host new phenomena and observables that would have been inaccessible in other systems. The results pose another significant step towards the dream of “topological photonics,” in which quantum Hall physics and other forms of topological behavior will provide the basis for photonic devices. This research is published in Physical Review Letters. FIG. 1: A schematic of the two-dimensional photonic crystal used by Soljačić’s group to demonstrate a photonic version of the quantum anomalous Hall effect. As a result of high Chern numbers, there are multiple photonic states propagating at the edge of the sample that are topologically protected from backscattering. (APS/Alan Stonebraker) ilar models have previously been realized in photonics [6, 8, 9], cold atomic systems [10], and condensed matter [11], but they were limited to Chern numbers of 1. By analyzing the dispersion curves of the modes propagating at the edge of the crystal, the group proved that the system behaves like a quantum anomalous Hall system with Chern numbers up to 4. This may give rise to effects and applications that would have been impossible for systems with Chern numbers of 1. For instance, information could be multiplexed over several spatial channels provided by the topological edge modes, leading to faster, higher-capacity, and more robust on-chip communication. Robust nonlinear mode conversion could be achieved by using nonlinear effects to mix the scatter-free modes. Finally, the authors show that the availability of multiple edge states allows a unique routing geometry, in which the states can be split at a corner and sent to different “ports.” Because of topological protection, this rerouting circuit wouldn’t suffer from any losses due to backscattering. But one of the most interesting aspects of the work lies in the entirely new experimental procedure used to map out the dispersion relation of the topological edge states. The authors’ method can be loosely seen as a photonic analog of photoemission spectroscopy—the method used to characterize the dispersion of two-dimensional electronic states on the surface of three-dimensional topological insulators. For two-dimensional systems, which have one-dimensional topological states at their edges, photoemission spectroscopy would be extremely challenging because an incoming optical probe beam cannot access an extremely thin one-dimensional edge. Two-dimensional quantum topological behavior has thus been typically characterized via transport measurements. The authors use microwave photons to provide a characterization similar to photoemission, as it can directly access the band structure of the one-dimensional edge states. They scanned the edges of the photonic crystal with microwaves—injected and collected by antennae—determining the amplitude and phase of the elecDOI: 10.1103/Physics.8.122 URL: http://link.aps.org/doi/10.1103/Physics.8.122 http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Physics American Physical Society (APS)

High Chern Numbers in Photonic Crystals

Rechtsman, Mikael C.
Physics , Volume 8: 1 – Dec 14, 2015
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References (9)

Publisher
American Physical Society (APS)
Copyright
© 2015 American Physical Society
Subject
VIEWPOINTS
ISSN
1943-2879
eISSN
1943-2879
DOI
10.1103/Physics.8.122
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Abstract

topological concepts to describe condensed-matter systems was first put forward in the description of the integer quantum Hall effect by David Thouless, Mahito Kohmoto, Peter Nightingale, and Marcel den Nijs [4]. They showed that the Hall conductance of a two-dimensional electron system under a large magnetic field can be quantized, that is, fixed to be an integer times a fundamental constant, e2 /h. That integer, DOI: 10.1103/Physics.8.122 URL: http://link.aps.org/doi/10.1103/Physics.8.122 known as the Chern number, corresponds to the number of edge states that carry current, without scattering, across the system. The Chern number indicates topological behavior in the sense that small deformations of the system (such as disorder, strain, and localized defects) have little effect on its properties. This makes the system’s physics independent of its minute details (such as hopping parameters, number of dopants, or atomic constituents) and only dependent on this global quantity, which must be an integer. In other words, it depends on the system’s topology rather than on its geometry. Although the initial interest in topological phenomena focused on electrons, topological behavior can be generalized to any type of wave, including light, as first predicted in Ref. [5]. A magnetic photonic crystal—a photonic crystal made of materials that break Lorentz reciprocity due to their response to an external magnetic field—can have a nonzero Chern number (and associated nonscattering edge states) for electromagnetic modes, that is, photons, rather than electrons. Soljačić’s group demonstrated this in 2009, showing that a topological protection of microwave photons could be observed in photonic crystals [6]. The finding launched a search for the realization of topological insulators for photons at optical wavelengths [7], motivated by the prospect of engineering robust optical devices, immune to disorder. Using similar mechanisms as in Ref. [6] proved challenging because of the weakness of magnetic effects in the optical regime. But alternative mechanisms later enabled robust topological edge states for light in a photonic lattice [8] and silicon ring resonator arrays [9]. Employing a microwave photonic crystal similar to the one they used previously [6], Soljačić’s team now reports another important discovery, that of high-Chern number (> 1) bands in a photonic quantum anomalous Hall system. The authors utilized a scheme (see Fig. 1) based on two-dimensional photonic crystals made of ferromagnetic garnet rods sandwiched between two copper plates. Simc 2015 American Physical Society tromagnetic field transmitted by the crystal. (An advantage of the microwave regime is that phase information is much easier to collect than in optics.) By Fourier transforming the spatial profile of the edge states, they determined their lattice momentum as a function of frequency, mapping out their band structure and determining the Chern numbers of each band. As a result of the higher-Chern-number bands, there are multiple edge states that cross the band gaps of the photonic crystal [2]. To my knowledge, the data collected by Soljačić’s team are the first direct experimental characterization of the band structure of a one-dimensional topological edge state. This work demonstrates the surprising generality of topological physics and the fact that alternative wavebased systems, such as photonics, can host new phenomena and observables that would have been inaccessible in other systems. The results pose another significant step towards the dream of “topological photonics,” in which quantum Hall physics and other forms of topological behavior will provide the basis for photonic devices. This research is published in Physical Review Letters. FIG. 1: A schematic of the two-dimensional photonic crystal used by Soljačić’s group to demonstrate a photonic version of the quantum anomalous Hall effect. As a result of high Chern numbers, there are multiple photonic states propagating at the edge of the sample that are topologically protected from backscattering. (APS/Alan Stonebraker) ilar models have previously been realized in photonics [6, 8, 9], cold atomic systems [10], and condensed matter [11], but they were limited to Chern numbers of 1. By analyzing the dispersion curves of the modes propagating at the edge of the crystal, the group proved that the system behaves like a quantum anomalous Hall system with Chern numbers up to 4. This may give rise to effects and applications that would have been impossible for systems with Chern numbers of 1. For instance, information could be multiplexed over several spatial channels provided by the topological edge modes, leading to faster, higher-capacity, and more robust on-chip communication. Robust nonlinear mode conversion could be achieved by using nonlinear effects to mix the scatter-free modes. Finally, the authors show that the availability of multiple edge states allows a unique routing geometry, in which the states can be split at a corner and sent to different “ports.” Because of topological protection, this rerouting circuit wouldn’t suffer from any losses due to backscattering. But one of the most interesting aspects of the work lies in the entirely new experimental procedure used to map out the dispersion relation of the topological edge states. The authors’ method can be loosely seen as a photonic analog of photoemission spectroscopy—the method used to characterize the dispersion of two-dimensional electronic states on the surface of three-dimensional topological insulators. For two-dimensional systems, which have one-dimensional topological states at their edges, photoemission spectroscopy would be extremely challenging because an incoming optical probe beam cannot access an extremely thin one-dimensional edge. Two-dimensional quantum topological behavior has thus been typically characterized via transport measurements. The authors use microwave photons to provide a characterization similar to photoemission, as it can directly access the band structure of the one-dimensional edge states. They scanned the edges of the photonic crystal with microwaves—injected and collected by antennae—determining the amplitude and phase of the elecDOI: 10.1103/Physics.8.122 URL: http://link.aps.org/doi/10.1103/Physics.8.122

Journal

Physics – American Physical Society (APS)

Published: Dec 14, 2015

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