Current state-of-the-art of pulsed laser deposition of optical waveguide structures: Existing capabilities and future trends

• Published in: Applied surface science Vol. 255; no. 10; pp. 5199 - 5205
• Main Authors: Eason, R.W., May-Smith, T.C., Grivas, C., Darby, M.S.B., Shepherd, D.P., Gazia, R.
• Format: Journal Article Conference Proceeding
• Language: English
• Published: Amsterdam Elsevier B.V 01.03.2009; Elsevier
• Subjects: Combinatorial; Condensed matter: electronic structure, electrical, magnetic, and optical properties; Condensed matter: structure, mechanical and thermal properties; Cross-disciplinary physics: materials science; rheology; Exact sciences and technology; Garnet crystal; Multilayers; Optical; Physics; Pulsed laser deposition; Waveguide; 78.20.−e; Garnet crystal; Multilayers; Optical; Combinatorial; 68.55.at; 77.84.Bw; Pulsed laser deposition; 81.15.Fg; 78.67.pt; Waveguide; 78.20.-e; Optical waveguides; Film growth; Garnets; Waveguides
• ISSN: 0169-4332; 1873-5584
• DOI: 10.1016/j.apsusc.2008.07.133

Pulsed laser deposition (PLD) has now reached a stage of maturity where the growth of thin films is routine. All that is required is a pulsed ultra-violet (UV) wavelength laser, a vacuum chamber, a target, and a substrate placed in near proximity to the plasma plume. Whether the film that you grow is the film that you need, and whether the thickness, uniformity, optical quality, stoichiometry, degree of crystallinity, orientation and much more is what is desired is another question entirely. PLD is both a science and an art and there are many tricks-of-the-trade that need to be considered to ensure that materials grown are the materials wanted. This paper discusses the practicalities of PLD systems, target geometries, heating regimes for successful epitaxial growth of crystalline films, the problem of particulates, laser sources to use, and in the context of our most recent PLD system, the number of independent lasers and targets used. We show that the use of multiple targets permits a combinatorial approach, whereby stoichiometry can be adjusted to grow designer materials, and in particular multilayer systems, ideally suited for active optical waveguides, a truly demanding end application where optical quality and in-plane losses must be reduced to an absolute minimum.