Abstract

We report the development of on-chip optical components designed to improve the out-coupling of double-metal terahertz (THz) frequency quantum cascade lasers (QCLs). A visible reshaping of the optical beam is achieved, independent of the precise waveguide configuration, by direct incorporation of cyclic-olefin copolymer (COC) dielectric optical fibers onto the QCL facet. A major improvement is further achieved by incorporating a micromachined feed-horn waveguide, assembled around the THz QCL and integrated with a slit-coupler. In its first implementation, we obtain a ± 20° beam divergence, offering the potential for high-efficiency radiation coupling from a metal-metal waveguide into optical fibers.

Highlights

  • Whilst the visible, infrared and microwave ranges of the electromagnetic spectrum benefit from established signal routing and processing components, the terahertz (THz) frequency range still requires a suitable framework of equivalent components

  • Low divergence double-metal devices have been realized over the last few years, principally by exploiting lithographic approaches based on engineering third-order distributed feedback gratings [8], plasmonic collimators [9], circular resonator approaches for vertical emission [10], photonic crystals [11] and quasi-crystals [12]

  • It is worth mentioning that the assembly of the waveguide coupler on the quantum cascade lasers (QCLs) is achieved by gluing it with photoresist, meaning that it is a reversible process which allows one to disassemble the coupler without damaging the QCL ridge by removing the photoresist with acetone

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Summary

Introduction

Whilst the visible, infrared and microwave ranges of the electromagnetic spectrum benefit from established signal routing and processing components, the terahertz (THz) frequency range still requires a suitable framework of equivalent components. One of the key issues in THz QCL technology is, the divergence of the outcoming beams: in a standard edge emitting configuration the radiation is emitted in a beam with approximately 30° divergence for single-plasmon waveguides [6], whereas an almost isotropic emission, rich in fringes, is seen for the case of double-metal [7] waveguides. This is principally due to diffraction at the subwavelength-sized laser facet, and interference between emissions from the two cleaved facets. Low divergence double-metal devices have been realized over the last few years, principally by exploiting lithographic approaches based on engineering third-order distributed feedback gratings [8], plasmonic collimators [9], circular resonator approaches for vertical emission [10], photonic crystals [11] and quasi-crystals [12]

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