Abstract

In recent years, nanolasers based on plasmonic crystal nanocavity structures have attracted significant interest. However, the performance of such lasers is affected significantly by the coupling of the lasing emission to both reflection and transmission sides of the device and to multiple spatial modes in the far field due to higher-order diffraction from plasmonic crystals as well. In this work, we propose a nanolaser design that overcomes the performance degradation of plasmonic crystal based nanolasers and increases the emission intensity significantly. In the proposed nanolaser structure, a nanometer-thick gain medium has a one-dimensional photonic crystal on one side and a metal nanohole array on the other side. An incident pump pulse through the one-dimensional photonic crystal excites optical Tamm states at the metal-gain medium interface that are amplified by the stimulated emission of the gain medium. We find that the intensity of the extraordinary optical transmission through the metal nanohole array increases significantly due to the excitation of optical Tamm states with wavevector perpendicular to the nanohole array surface. We also find that the subwavelength periodicity in the nanohole array confines the lasing emission to the zero-th order mode only, and hence, makes the far-field pattern highly directional. Moreover, the laser emission wavelength can be tuned over a broad range by changing the thicknesses of the photonic crystal layers, gain medium, and in real-time, by changing the angle of incidence of the pump pulse.

Highlights

  • Nanoscale manipulation of light has led to drastic miniaturization of many optical devices such as bio-sensors, solar cells, and photodetectors

  • Upon further investigation of the population densities of the structure, we find that the gain medium reaches population inversion with a silica nanohole array (NHA) when the pump pulse has an energy of 0.026 mJ cm−2, but fails to support lasing emission as the silica NHA cannot provide sufficient feedback essential for lasing action

  • The stimulated emission from the gain medium couples to localized surface plasmon (LSP) in the NHA so that light can be confined in a nanoscale cavity

Read more

Summary

Introduction

Nanoscale manipulation of light has led to drastic miniaturization of many optical devices such as bio-sensors, solar cells, and photodetectors. The stimulated emission from the gain medium couples to resonant SPP-Bloch modes resulting in amplification and lasing, and a highly directional far-field emission profile. At visible wavelength, such metal hole array based lasers have produced far-field emission profiles with a divergence angle of ∼1–3° [20]. Unidirectional lasing has been achieved using template-stripped twodimensional plasmonic crystals, where optically thick gold (Au) substrate reflects lasing emission onto the same side as the pump source [22] Such a structure suffers from the complexity related to separating the lasing emission from the incident light, increased ohmic losses in the metal layer, and lack of far-field directionality of lasing emission. The proposed nanolaser can be tuned dynamically by changing the incident angle of the pump pulse

Design and simulation
Cavity dynamics
Emission characteristics
Tuning emission spectra
Findings
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call