4.8 Article

Scalable single-mode surface-emitting laser via open-Dirac singularities

Journal

NATURE
Volume 608, Issue 7924, Pages 692-+

Publisher

NATURE PORTFOLIO
DOI: 10.1038/s41586-022-05021-4

Keywords

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Funding

  1. Office of Naval Research (ONR) Young Investigator Award [N00014-19-1-2737]
  2. ONR JTO MRI Award [N00014-20-1-2752]
  3. ONR [N00014-20-1-2723]
  4. National Science Foundation (NSF) Career Award [ECCS-1929659]
  5. Laboratory Directed Research and Development Program of Lawrence Berkeley National Laboratory (LBNL) under US Department of Energy [DE-AC02-05CH11231]
  6. NSF QLCI programme [OMA-2016245]
  7. Bakar Fellowship at UC Berkeley
  8. National Science Foundation [ECCS-1542148]
  9. Moore Inventor Fellows programme

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In this study, the authors propose and demonstrate the existence of open-Dirac electromagnetic cavities that exhibit scale invariant single-mode lasing. The physical mechanism behind this phenomenon lies in the convergence of the complex part of the free spectral range in open-Dirac cavities towards a constant, determined by the loss rates of different Bloch bands. The authors name these sources Berkeley surface-emitting lasers (BerkSELs) and show that their far-field corresponds to a topological singularity of charge two.
Single-aperture cavities are a key component of lasers that are instrumental for the amplification and emission of a single light mode. However, the appearance of high-order transverse modes as the size of the cavities increases has frustrated efforts to scale-up cavities while preserving single-mode operation since the invention of the laser six decades ago(1-8). A suitable physical mechanism that allows single-mode lasing irrespective of the cavity size-a 'scale invariant' cavity or laser-has not been identified yet. Here we propose and demonstrate experimentally that open-Dirac electromagnetic cavities with linear dispersion-which in our devices are realized by a truncated photonic crystal arranged in a hexagonal pattern-exhibit unconventional scaling of losses in reciprocal space, leading to single-mode lasing that is maintained as the cavity is scaled up in size. The physical origin of this phenomenon lies in the convergence of the complex part of the free spectral range in open-Dirac cavities towards a constant governed by the loss rates of distinct Bloch bands, whereas for common cavities it converges to zero as the size grows, leading to inevitable multimode emission. An unconventional flat-envelope fundamental mode locks all unit cells in the cavity in phase, leading to single-mode lasing. We name such sources Berkeley surface-emitting lasers (BerkSELs) and demonstrate that their far-field corresponds to a topological singularity of charge two, in agreement with our theory. Open-Dirac cavities unlock avenues for light-matter interaction and cavity quantum electrodynamics.

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