Distributed Feedback Lasers Based on Green Fluorescent Protein and Conformal High Refractive Index Oxide Layers. Issue 6 (19th May 2020)

• Record Type: Journal Article
• Authors: Karl, Markus; Meek, Andrew; Murawski, Caroline; Tropf, Laura; Keum, Changmin; Schubert, Marcel; Samuel, Ifor D. W.; Turnbull, Graham A.; Gather, Malte C.
• Is Part Of: Laser & photonics reviews. Volume 14:Issue 6(2020)
• Page Start: n/a
• Page End: n/a
• Publication Date: 2020-05-19
• Subjects: biolasers, atomic layer deposition (ALD) -- distributed feedback (DFB) -- far‐field mode analysis -- fluorescent proteins -- tunable lasing; Lasers -- Periodicals; Photonics -- Periodicals; Lasers -- Périodiques; Photonique -- Périodiques; 621.36
• DOI: 10.1002/lpor.202000101
• Languages: English
• ISSNs: 1863-8880

Abstract

Abstract: Fluorescent proteins have emerged as an attractive gain material for lasers, especially for devices requiring biocompatibility. However, due to their optical properties, integration with distributed feedback (DFB) resonators is not readily achievable. Here, a DFB laser with enhanced green fluorescent protein (eGFP) as the gain material is demonstrated by incorporating a thin (65 nm), high refractive index ( n = 2.12) ZrO2 interlayer as waveguide core. Deposition of ZrO2 via atomic layer deposition yields a smooth and conformal film as required to minimize optical losses. Lasing emission is obtained from 2D second‐order DFB eGFP lasers at pump power densities above 56.6 kW cm –2 and a wavelength tuning range of Δ λ = 51.7 nm is demonstrated. Furthermore, it is shown that in contrast to conventional organic DFB lasers, both transverse electric (TE) and transverse magnetic (TM) modes are accessible. The effective refractive index of these modes can be predicted accurately through optical modelling. Using far‐field imaging, the laser beam profile is studied and TE and TM modes are distinguished. Abstract : The biologically produced green fluorescent protein (GFP) is employed as a gain medium in distributed feedback lasers. Insertion of a thin, high‐index waveguide core permits usage of a GFP layer in an efficient evanescent gain configuration. The lasing threshold under ns‐excitation is below 60 kW cm −2 . The lasing wavelength can be tuned over more than 50 nm.