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Photonic bands in two-dimensionally patterned multimode GaN waveguides for light extraction
3.M. R. Krames, M. Ochiai-Holcomb, G. E. Holfer, C. Carter-Coman, E. I. Chen, I. H. Tan, P. Grillot, N. F. Gardner, H. C. Chui, J. W. Huang, S. A. Stockman, F. A. Kish, M. G. Craford, S. T. Tan, C. P. Kocot, M. Hueschen, J. Posselt, B. Loh, G. Sasser, and D. Collins, Appl. Phys. Lett. 75, 2365 (1999).
5.J. J. Wierer, M. R. Krames, J. E. Epler, N. F. Gardner, M. G. Craford, J. R. Wendt, J. A. Simmons, and M. M. Sigalas, Appl. Phys. Lett. 84, 3885 (2004).
8.M. Rattier, H. Benisty, R. P. Stanley, J.-F. Carlin, R. Houdré, U. Oesterle, C. J.M. Smith, C. Weisbuch, and T. F. Krauss, IEEE J. Sel. Top. Quantum Electron. 8, 238 (2002).
9.H. Rigneault, F. Lemarchand, and A. Sentenac, J. Opt. Soc. Am. A 17, 1048 (2000).
10.R. K. Lee, Y. Xu, and A. Yariv, J. Opt. Soc. Am. B 17, 1438 (2000).
11.This choice is due to the sixfold symmetry of the triangular lattice, which should display quite isotropic behavior and constitute a first step towards omnidirectional extraction. Further study of the directionality issue will be reported elsewhere.
13.S. G. Johnson, P. Bienstman, M. A. Skorobogatiy, M. Ibanescu, E. Lidorikis, and J. D. Joannopoulos, Phys. Rev. E 66, 06608 (2002).
14.M. Rattier, H. Benisty, E. Schwoob, C. Weisbuch, T. F. Krauss, C. J.M. Smith, R. Houdre, and U. Oesterle, Appl. Phys. Lett. 83, 1283 (2003).
16.More precisely, the light is diffracted in the left half space, with an azimuthal direction depending on the (small) incident angle of the guided mode with respect to the direction. Angular measurements slightly off the direction reveal similar results as those reported.
17.In our method, designed to account for losses by diffraction, the electric field is decomposed in a plane wave basis along the periodic directions of the PhC, and discretized in real space in the vertical direction. The frequency of light is imposed, and Maxwell’s equations take the form of an eigenvalue problem where we solve for the wave vector and Bloch mode profile. Details will be published elsewhere.
18.H. Y. Zhang, X. H. He, Y. H. Shih, M. Schurman, Z. C. Feng, and R. A. Stall, Opt. Lett. 21, 1529 (1996).
19.Due to the directionality of the incoming guided modes, B-modes would not be excited as they stem from guided modes propagating off the direction.
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