[1] E. Yablonovitch. Inhibited spontaneous emission in solid-state physics and electronics. Phys. Rev. Lett., 1987, 58(20): 2059-2062.

[2] S. John. Strong localization of photons in certain disordered dielectric superlattices. Phys. Rev. Lett., 1987, 58(23): 2486-2489.

[3] A. Blanco, et al.. Large-scale synthesis of a silicon photonic crystal with a complete three-dimensional bandgap near 1.5 micrometres. Nature, 2000, 405: 437-440.

[4] K. M. Ho, C. T. Chan, C. M. Soukoulis. Existence of a photonic gap in periodic dielectric structures. Phys. Rev. Lett., 1990, 65(25): 3152-3155.

[5] J. B. Pendry, et al.. Extremely low frequency plasmons in metallic mesostructures. Phys. Rev. Lett., 1996, 76(25): 4773-4776.

[6] E. Yablonovitch, et al.. Donor and acceptor modes in photonic band structure. Phys. Rev. Lett., 1991, 67(24): 3380-3383.

[7] O. Painter, et al.. Two-dimensional photonic band-gap defect mode laser. Science, 1999, 284(5421): 1819-1821.

[8] M. Notomi. Manipulating light with strongly modulated photonic crystals. Rep. Prog. Phys., 2010, 73(9): 096501.

[9] N. Yu, F. Capasso. Flat optics with designer metasurfaces. Nat. Mater., 2014, 13: 139-150.

[10] A. Arbabi, et al.. Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission. Nat. Nanotechnol., 2015, 10(11): 937-943.

[11] J. S. T. Smalley, et al.. Luminescent hyperbolic metasurfaces. Nat. Commun., 2017, 8: 13793.

[12] A. I. Kuznetsov, et al.. Optically resonant dielectric nanostructures. Science, 2016, 354(6314): aag2472.

[13] I. V.Shadrivov, M.Lapine and Y. S.Kivshar, Nonlinear, Tunable and Active Metamaterials, Springer, Cham, Switzerland (2015).

[14] S. Longhi. Quantum-optical analogies using photonic structures. Laser Photonics Rev., 2009, 3(3): 243-261.

[15] A. H. C. Neto, et al.. The electronic properties of graphene. Rev. Mod. Phys., 2009, 81(1): 109-162.

[16] S. Raghu, F. D. M. Haldane. Analogs of quantum-Hall-effect edge states in photonic crystals. Phys. Rev. A, 2008, 78(3): 033834.

[17] R. A. Sepkhanov, Y. B. Bazaliy, C. W. Beenakker. Extremal transmission at the Dirac point of a photonic band structure. Phys. Rev. A, 2007, 75(6): 063813.

[18] O. Bahat-Treidel, et al.. Klein tunneling in deformed honeycomb lattices. Phys. Rev. Lett., 2010, 104(8): 063901.

[19] O. Bahat-Treidel, O. Peleg, M. Segev. Symmetry breaking in honeycomb photonic lattices. Opt. Lett., 2008, 33(19): 2251-2253.

[20] O. Peleg, et al.. Conical diffraction and gap solitons in honeycomb photonic lattices. Phys. Rev. Lett., 2007, 98(10): 103901.

[21] M. J. Ablowitz, S. D. Nixon, Y. Zhu. Conical diffraction in honeycomb lattices. Phys. Rev. A, 2009, 79(5): 053830.

[22] H. Kogelnik, C. V. Shank. Stimulated emission in a periodic structure. Appl. Phys. Lett., 1971, 18: 152-154.

[23] C. V. Shank, J. E. Bjorkholm, H. Kogelnik. Tunable distributed-feedback dye laser. Appl. Phys. Lett., 1971, 18(9): 395-396.

[24] M. Meier, et al.. Laser action from two-dimensional distributed feedback in photonic crystals. Appl. Phys. Lett., 1999, 74(1): 7-9.

[25] W. Zhou, et al.. Lasing action in strongly coupled plasmonic nanocavity arrays. Nat. Nanotechnol., 2013, 8(7): 506-511.

[26] M. Karl, et al.. Flexible and ultra-lightweight polymer membrane lasers. Nat. Commun., 2018, 9(1): 1525.

[27] L. Ju, et al.. Graphene plasmonics for tunable terahertz metamaterials. Nat. Nanotechnol., 2011, 6(10): 630-634.

[28] S. Xiao, et al.. Tunable magnetic response of metamaterials. Appl. Phys. Lett., 2009, 95(3): 033115.

[29] Z. Li, et al.. Mechanically tunable optofluidic distributed feedback dye laser. Opt. Express, 2006, 14(22): 10494-10499.

[30] D. Psaltis, S. R. Quake, C. Yang. Developing optofluidic technology through the fusion of microfluidics and optics. Nature, 2006, 442: 381-386.

[31] K. Busch, S. John. Liquid-crystal photonic-band-gap materials: the tunable electromagnetic vacuum. Phys. Rev. Lett., 1999, 83(5): 967-970.

[32] A. Bakal, et al.. Tunable on chip optofluidic laser. Appl. Phys. Lett., 2015, 107(21): 211105.

[33] V. N. Smolyaninova, et al.. Self-assembled tunable photonic hyper-crystals. Sci. Rep., 2015, 4: 5706.

[34] M. Gersborg-Hansen, A. Kristensen. Tunability of optofluidic distributed feedback dye lasers. Opt. Express, 2007, 15(1): 137-142.

[35] F. B. Arango, et al.. Optofluidic tuning of photonic crystal band edge lasers. Appl. Phys. Lett., 2007, 91(22): 223503.

[36] S. Rubin, Y. Fainman. Nonlocal and nonlinear surface plasmon polaritons and optical spatial solitons induced by the thermocapillary effect. Phys. Rev. Lett., 2018, 120(24): 243904.

[37] S. Rubin, B. Hong, Y. Fainman. Subnanometer imaging and controlled dynamical patterning of thermocapillary driven deformation of thin liquid films. Light Sci. Appl., 2019, 8(1): 1-11.

[38] V. G.Levich, Physicochemical Hydrodynamics, Prentice Hall, Englewood Cliffs, New Jersey (1962).

[39] H. M. J. M. Wedershoven, et al.. Infrared laser induced rupture of thin liquid films on stationary substrates. Appl. Phys. Lett., 2014, 104(5): 054101.

[40] J. Muller, H. M. J. M. Wedershoven, A. A. Darhuber. Monitoring photochemical reactions using Marangoni flows. Langmuir, 2017, 33(15): 3647-3658.

[41] H.Raether, Surface Plasmons on Smooth and Rough Surfaces and on Gratings, Springer-Verlag, Berlin (2013).

[42] H.Kogelnik, “Theory of optical waveguides,” in Guided-Wave Optoelectronics, and T.Tamir, Eds., Vol. 26, pp. 13–81, Springer Series in Electronics and Photonics, Springer, Berlin, Heidelberg (1975).

[43] V. V. Yaminsky, et al.. Stability of aqueous films between bubbles. Part 1. The effect of speed on bubble coalescence in purified water and simple electrolyte solutions. Langmuir, 2010, 26(11): 8061-8074.

[44] A.Patsyket al., “Observation of branched flow of light,” in CLEO: QELS Fundamental Sci., Optical Society of America (2019).

[45] Y. Lamhot, et al.. Optical control of thermocapillary effects in complex nanofluids. Phys. Rev. Lett., 2009, 103(26): 264503.

[46] J.Happel and H.Brenner, Low Reynolds Number Hydrodynamics, pp. 431–441, Martinus Nijhoff, The Hague (1983).

[47] I. S. Aranson, L. Kramer. The world of the complex Ginzburg–Landau equation. Rev. Mod. Phys., 2002, 74: 99-143.

[48] A. Marini, D. V. Skryabin. Ginzburg–Landau equation bound to the metal–dielectric interface and transverse nonlinear optics with amplified plasmon polaritons. Phys. Rev. A, 2010, 81(3): 033850.

[49] A. Davoyan, et al.. Nonlinear nanofocusing in tapered plasmonic waveguides. Phys. Rev. Lett., 2010, 105(11): 116804.

[50] H. J.Eichleret al., Laser-Induced Dynamic Gratings, Vol. 50, Springer, Berlin (2013).

[51] P. R. Wallace. The band theory of graphite. Phys. Rev., 1947, 71(9): 622-634.

[52] G.Lifante, Integrated Photonics: Fundamentals, John Wiley & Sons, Hoboken, New Jersey (2003).

[53] T.Suhara, Semiconductor Laser Fundamentals, CRC Press, Boca Raton, Florida (2004).

[54] H. Kogelnik, C. V. Shank. Coupled-wave theory of distributed feedback lasers. J. Appl. Phys., 1972, 43(5): 2327-2335.

[55] A.Yariv and P.Yeh, Photonics: Optical Electronics in Modern Communications, Oxford University Press, Oxford (2006).

[56] J. M.Liu, Photonic Devices, Cambridge University Press, Cambridge (2009).

[57] M. J. Ablowitz, Y. Zhu. Evolution of Bloch-mode envelopes in two-dimensional generalized honeycomb lattices. Phys. Rev. A, 2010, 82(1): 013840.

[58] M. J. Ablowitz, Y. Zhu. Nonlinear wave packets in deformed honeycomb lattices. SIAM J. Appl. Math., 2013, 73(6): 1959-1979.

[59] M. I. Shalaev, et al.. Reconfigurable topological photonic crystal. New J. Phys., 2018, 20(2): 023040.

[60] K. E. Oughstun, N. A. Cartwright. On the Lorentz–Lorenz formula and the Lorentz model of dielectric dispersion. Opt. Express, 2003, 11(13): 1541-1546.

[61] S.-L. Zhu, B. Wang, L.-M. Duan. Simulation and detection of Dirac fermions with cold atoms in an optical lattice. Phys. Rev. Lett., 2007, 98(26): 260402.

[62] L. Tarruell, et al.. Creating, moving and merging Dirac points with a Fermi gas in a tunable honeycomb lattice. Nature, 2012, 483: 302-305.

[63] N. M. Estakhri, B. Edwards, N. Engheta. Inverse-designed metastructures that solve equations. Science, 2019, 363(6433): 1333-1338.

[64] A. Oron, S. H. Davis, S. G. Bankoff. Long-scale evolution of thin liquid films. Rev. Mod. Phys., 1997, 69(3): 931-980.

[65] S.Hassani, Mathematical Physics: A Modern Introduction to Its Foundations, Springer Science & Business Media, Berlin (2013).