Nonplanar nanoselective area growth of InGaAs/InP

In this study, we have investigated metal-organic vapor phase epitaxial nano-patterned selective area growth of InGaAs/InP on non-planar (001) InP surfaces. Due to high etching resistance and the small molecular size of negative tone electron beam HSQ resist, the protection mask formed in HSQ has small feature sizes in ten nanometers scale and allow realization of in-situ etching. As was observed in the SAG regime, in-situ etching of InP by carbon tetrabromide leads to formation of self-limited structures. By altering etching time, the groove shape can be changed from a triangular trench to a trapeze. Another appealing aspect of in situ etching is that the shape of InGaAs can be tuned from a crescent to a triangular or a line by varying growth parameters. Quantum well wires can be fabricated by growing directly in the bottom of V-shaped groove. In addition, changes of mask orientations lead to anistropic or isotropic character of etching. The investigated technique of nano-patterned selective area growth allows obtaining different profiles of structures and different quantum structures such as quantum well or wires in the same growth run. To investigate the shape and crystalline quality of the active material, the cross-sectional geometry was observed by field emission scanning electron microscopy and scanning transmission electron microscopy. The optical properties were carried out at room temperature using micro-photoluminescence setup. The results showed different deposition rates for openings oriented along [0-11] and [0-1-1] directions with higher rate along [0-1-1]. The fabricated active material was incorporated into photonic crystal waveguides.

[1]  N. Gogneau,et al.  One-step nano-selective area growth (nano-SAG) of localized InAs/InP quantum dots: First step towards single-photon source applications , 2008 .

[2]  C. W. Hagen,et al.  Resists for sub-20-nm electron beam lithography with a focus on HSQ: state of the art , 2009, Nanotechnology.

[3]  David A. B. Miller,et al.  Device Requirements for Optical Interconnects to Silicon Chips , 2009, Proceedings of the IEEE.

[4]  Jeff F. Young,et al.  Extrinsic optical scattering loss in photonic crystal waveguides: role of fabrication disorder and photon group velocity. , 2005, Physical review letters.

[5]  Yun Sun,et al.  Optimized cleaning method for producing device quality InP(100) surfaces , 2005 .

[6]  Dan Dalacu,et al.  Broadband Purcell factor enhancements in photonic-crystal ridge waveguides , 2009 .

[7]  J. Décoberta,et al.  Modeling and characterization of AlGaInAs and related materials using selective area growth by metal-organic vapor-phase epitaxy , 2007 .

[8]  Steven G. Johnson,et al.  Block-iterative frequency-domain methods for Maxwell's equations in a planewave basis. , 2001, Optics express.

[9]  A. Rudra,et al.  Growth temperature dependence of the interfacet migration in chemical beam epitaxy of InP on non-planar substrates , 1996 .

[10]  R. E. Mallard,et al.  Selective-area low-pressure MOCVD of GaInAsP and related materials on planar InP substrates , 1993 .

[11]  M. Notomi,et al.  Ultralow Operating Energy Electrically Driven Photonic Crystal Lasers , 2013, IEEE Journal of Selected Topics in Quantum Electronics.

[12]  Gerald B. Stringfellow,et al.  Organometallic Vapor-Phase Epitaxy , 1989 .

[13]  Andreas Schlachetzki,et al.  InGaAs quantum wires and wells on V-grooved InP substrates , 1999 .

[14]  D. Bimberg,et al.  InGaAs quantum wires grown by low pressure metalorganic chemical vapor deposition on InP V‐grooves , 1996 .