Hydride vapour phase epitaxy assisted buried heterostructure quantum cascade lasers for sensing applications

Buried heterostructure (BH) lasers are routinely fabricated for telecom applications. Development of quantum cascade lasers (QCL) for sensing applications has largely benefited from the technological achievements established for telecom lasers. However, new demands are to be met with when fabricating BH-QCLs. For example, hetero-cascade and multistack QCLs, with several different active regions stacked on top of each other, are used to obtain a broad composite gain or increased peak output power. Such structures have thick etch ridges which puts severe demand in carrying out regrowth of semi-insulating layer around very deeply etched (< 10 μm) ridges in short time to realize BH-QCL. For comparison, telecom laser ridges are normally only <5 μm deep. We demonstrate here that hydride vapour phase epitaxy (HVPE) is capable of meeting this new demand adequately through the fabrication of BH-QCLs in less than 45 minutes for burying ridges etched down to 10-15 μm deep. This has to be compared with the normally used regrowth time of several hours, e.g., in a metal organic vapour phase epitaxy (MOVPE) reactor. This includes also micro-stripe lasers resembling grating-like ridges for enhanced thermal dissipation in the lateral direction. In addition, we also demonstrate HVPE capability to realize buried heterostructure photonic crystal QCLs for the first time. These buried lasers offer flexibility in collecting light from the surface and relatively facile device characterization feasibility of QCLs in general; but the more important benefits of such lasers are enhanced light matter interaction leading to ultra-high cavity Q-factors, tight optical confinement, possibility to control the emitted mode pattern and beam shape and substantial reduction in laser threshold.

[1]  J. Faist,et al.  Quantum Cascade Laser , 1994, Science.

[2]  Sebastian Lourdudoss,et al.  Analysis of regrowth evolution around VCSEL type mesas , 2000 .

[3]  M. Carras,et al.  Effect of emitter number on quantum cascade laser monolithic phased array. , 2012, Optics letters.

[4]  Scott W. Corzine,et al.  High-temperature continuous wave operation of strain-balanced quantum cascade lasers grown by metal organic vapor-phase epitaxy , 2006 .

[5]  Manijeh Razeghi,et al.  Quantum cascade lasers that emit more light than heat , 2010 .

[6]  B. Simozrag,et al.  High thermal performance of μ-stripes quantum cascade laser , 2012 .

[7]  Xavier Marcadet,et al.  Coherent quantum cascade laser micro-stripe arrays , 2011 .

[8]  Mykhaylo P. Semtsiv,et al.  Semi-insulating InP:Fe for buried-heterostructure strain-compensated quantum-cascade lasers grown by gas-source molecular-beam epitaxy , 2013 .

[9]  Mykhaylo P. Semtsiv,et al.  Buried-heterostructure quantum-cascade laser overgrown by gas-source molecular-beam epitaxy , 2012 .

[10]  Wondwosen Metaferia,et al.  Demonstration of a quick process to achieve buried heterostructure quantum cascade laser leading to high power and wall plug efficiency , 2014 .

[11]  Manijeh Razeghi,et al.  Room temperature quantum cascade lasers with 27% wall plug efficiency , 2011 .

[12]  E. Gini,et al.  Buried heterostructure quantum cascade lasers with a large optical cavity waveguide , 2000, IEEE Photonics Technology Letters.

[13]  Mattias Beck,et al.  Buried heterostructure quantum cascade lasers , 1998, Photonics West.

[14]  Maria Maragkou Quantum cascade lasers: 2D photonic crystal laser , 2014 .

[15]  Mattias Beck,et al.  Continuous Wave Operation of a Mid-Infrared Semiconductor Laser at Room Temperature , 2001, Science.

[16]  Mattias Beck,et al.  Electrically tunable, high performance quantum cascade laser , 2010 .