Abstract

Triply-degenerate Dirac-like cone at the Brillouin zone center attracts much research interest in recent years. Whether the linear dispersion in such a Dirac-like cone reflects the same physics to Dirac cones at the Brillouin zone boundaries is still under investigation. In this manuscript, through microwave experiments and numerical simulations, we observe intriguing pulse reshaping phenomena in double-zero-index photonic crystals, which cannot be fully understood from their close-to-zero effective parameters. A reshaped pulse, with frequency components close to the Dirac frequency filtered, is propagating at a constant group velocity while part of these filtered frequencies appears at a much later time. In time domain measurements, we find a way to separate the effect between the linear dispersion and the extra flat band in Dirac-like cone to have a better understanding of the underneath physics. We succeed in obtaining the group velocity inside a double-zero-index photonic crystal and good consistence can be found between experiments, numerical simulations and band diagram calculations.

Highlights

  • In graphene, the conduction and valence bands touch each other at a singular point, Dirac point, and a conical band diagram, Dirac cone, is formed at the Brillouin zone (BZ) boundary

  • For photonic crystals (PCs) with Dirac cones at the BZ boundaries, as the density of states at the Dirac point is limited, transmission through a finite-thickness sample is limited as well[1,10], which means that the filtering effect as in pulse (1) is totally understandable

  • What is different here, from our pulse transmission experiment, is that the frequency components close to Dirac frequency ωD transmit through our DZI PC at a later time, whose frequency components are consistent with those of the extra flat band intersecting the Dirac cone at the Dirac point

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Summary

Introduction

The conduction and valence bands touch each other at a singular point, Dirac point, and a conical band diagram, Dirac cone, is formed at the Brillouin zone (BZ) boundary. What is different here, from our pulse transmission experiment, is that the frequency components close to Dirac frequency ωD transmit through our DZI PC at a later time, whose frequency components are consistent with those of the extra flat band intersecting the Dirac cone at the Dirac point.

Results
Conclusion
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