[1] PartoM.WittekS.HodaeiH.HarariG.BandresM. A.RenJ.RechtsmanM. C.SegevM.ChristodoulidesD. N.KhajavikhanM., “Complex edge-state phase transitions in 1D topological laser arrays,” arXiv: 1709.00523 (2017).

[2] J. Sun, E. Timurdogan, A. Yaacobi, E. S. Hosseini, M. R. Watts. Large-scale nanophotonic phased array. Nature, 2013, 493: 195-199.

[3] C. T. DeRose, R. D. Kekatpure, D. C. Trotter, A. Starbuck, J. R. Wendt, A. Yaacobi, M. R. Watts, U. Chettiar, N. Engheta, P. S. Davids. Electronically controlled optical beam-steering by an active phased array of metallic nanoantennas. Opt. Express, 2013, 21: 5198-5208.

[4] T. Komljenovic, R. Helkey, L. Coldren, J. E. Bowers. Sparse aperiodic arrays for optical beam forming and LIDAR. Opt. Express, 2017, 25: 2511-2528.

[5] C. A. Valagiannopoulos, V. Kovanis. Judicious distribution of laser emitters to shape the desired far-field patterns. Phys. Rev. A, 2017, 95: 063806.

[6] OsherS.FedkiwR., Level Set Methods and Dynamic Implicit Surfaces (Springer, 2003).

[7] M. Gustafsson, C. Sohl, G. Kristensson. Physical limitations on antennas of arbitrary shape. Proc. R. Soc. A, 2007, 463: 2589-2607.

[8] MillerO., “Photonic design: from fundamental solar cell physics to computational inverse design,” Ph.D. thesis (University of California, 2013).

[9] G. Kriehn, A. Kiruluta, P. E. Silveira, S. Weaver, S. Kraut, K. Wagner, R. T. Weverka, L. Griffiths. Optical BEAMTAP beamforming and jammer-nulling system for broadband phased-array antennas. Appl. Opt., 2000, 39: 212-230.

[10] J. Zhang, N. Liu, L. Zhang, S. Zhao, Y. Zhao. Active jamming suppression based on transmitting array designation for colocated multiple-input multiple-output radar. IET Radar Sonar Navig., 2016, 10: 500-505.

[11] N. Jablon. Adaptive beamforming with the generalized sidelobe canceller in the presence of array imperfections. IEEE Trans. Antennas Propag., 1986, 34: 996-1012.

[12] B. Widrow, K. M. Duvall, R. P. Gooch, W. C. Newman. Signal cancellation phenomena in adaptive antennas: causes and cures. IEEE Trans. Antennas Propag., 1982, 30: 469-478.

[13] A. Alù, N. Engheta. Cloaking a sensor. Phys. Rev. Lett., 2009, 102: 233901.

[14] C. A. Valagiannopoulos, P. Alitalo. Electromagnetic cloaking of cylindrical objects by multilayer or uniform dielectric claddings. Phys. Rev. B, 2012, 85: 115402.

[15] AlitaloP.ValagiannopoulosC. A.TretyakovS. A., “Simple cloak for antenna blockage reduction,” in IEEE International Symposium on Antennas and Propagation (2011).

[16] M. Selvanayagam, G. V. Eleftheriades. Experimental demonstration of active electromagnetic cloaking. Phys. Rev. X, 2013, 3: 041011.

[17] F. Monticone, A. Alù. Do cloaked objects really scatter less?. Phys. Rev. X, 2013, 3: 041005.

[18] M. H. Teimourpour, L. Ge, D. N. Christodoulides, R. El-Ganainy. Non-Hermitian engineering of single mode two dimensional laser arrays. Sci. Rep., 2016, 6: 33253.

[19] M. H. Teimourpour, A. Rahman, K. Srinivasan, R. El-Ganainy. Non-Hermitian engineering of synthetic saturable absorbers for applications in photonics. Phys. Rev. Appl., 2017, 7: 014015.

[20] K. G. Makris, Z. H. Musslimani, D. N. Christodoulides, S. Rotter. Constant-intensity waves and their modulation instability in non-Hermitian potentials. Nat. Commun., 2015, 6: 7257.

[21] A. Gao, S. T. M. Fryslie, B. J. Thompson, P. S. Carney, K. D. Choquette. Parity-time symmetry in coherently coupled vertical cavity laser arrays. Optica, 2017, 4: 323-329.

[22] Y. Kominis, V. Kovanis, T. Bountis. Controllable asymmetric phase-locked states of the fundamental active photonic dimer. Phys. Rev. A, 2017, 96: 043836.

[23] W. Liu, M. Li, R. S. Guzzon, E. J. Norberg, J. S. Parker, M. Lu, L. A. Coldren, J. Yao. An integrated parity-time symmetric wavelength-tunable single-mode microring laser. Nat. Commun., 2017, 8: 15389.

[24] O. Hess, E. Scholl. Spatio-temporal dynamics in twin-stripe semiconductor lasers. Physica D, 1994, 70: 165-177.

[25] R. Lang, K. Kobayashi. External optical feedback effects on semiconductor injection laser properties. IEEE J. Quantum Electron., 1980, 16: 347-355.

[26] G. Lythe, T. Erneux, A. Gavrielides, V. Kovanis. Low pump limit of the bifurcation to periodic intensities in a semiconductor laser subject to external optical feedback. Phys. Rev. A, 1997, 55: 4443-4448.

[27] C. A. Valagiannopoulos. A novel methodology for estimating the permittivity of a specimen rod at low radio frequencies. J. Electromagn. Waves. Appl., 2010, 24: 631-640.

[28] C. A. Valagiannopoulos. On examining the influence of a thin dielectric strip posed across the diameter of a penetrable radiating cylinder. Prog. Electromagn. Res. C, 2008, 3: 203-214.

[29] AbramowitzM.StegunI. A., Handbook of Mathematical Functions (National Bureau of Standards, 1970), pp. 360–361.

[30] JonesD. S., Theory of Electromagnetism (Pergamon, 1964), pp. 269–271.

[31] A. Andryieuski, A. V. Lavrinenko, M. Petrov, S. A. Tretyakov. Homogenization of metasurfaces formed by random resonant particles in periodical lattices. Phys. Rev. B, 2016, 93: 205127.

[32] BowersJ. E., “Evolution of photonic integrated circuits,” in 75th Annual Device Research Conference (2017).

[33] Y.-C. Xin, Y. Li, V. Kovanis, A. L. Gray, L. Zhang, L. F. Lester. Reconfigurable quantum dot monolithic multisection passive mode-locked lasers. Opt. Express, 2007, 15: 7623-7633.

[34] K. Sayyah, O. Efimov, P. Patterson, J. Schaffner, C. White, J.-F. Seurin, G. Xu, A. Miglo. Two-dimensional pseudo-random optical phased array based on tandem optical injection locking of vertical cavity surface emitting lasers. Opt. Express, 2015, 23: 19405-19416.