參考文獻 |
第一章
[1.1] S. E. Miller, A. G. Chynoweth: Optical Fiber Communications (Academic, New York 1979) Chap. 1.
[1.2] R. N. Hall, G. E. Fenner, J. D. Kingsley, T. J. Soltys, and R. O. Carlson, “Coherent light emission from GaAs juctions,” Phys. Rev. Lett. 9, 366-369 (1962).
[1.3] A. Yariv: Optical Electronics, 4th edn. (Holt, Rinehart and Winston, New York 1991) pp. 309-316.
[1.4] D. P. Schinke, R. G. Smith, A. R. Hartmann: Photodetectors, in Semiconductor Devices for Optical Communication, 2nd edn. (Springer, Berlin, Heidelberg 1980) Chap. 3.
[1.5] G. P. Aqrawal: Fiber-Optic Communication System (John Wiley & Sons, New York 2002).
[1.6] R. W. Ziolkowski and J. B. Judkins, “Full-wave vector Maxwell equation modeling of the self-focusing of ultrashort optical pulses in a nonlinear Kerr medium exhibiting a finite response time,” J. Opt. Soc. Am. B 10, 186-198 (1993).
[1.7] J. Donegan, “Two-photon absorption speeds optical switching,” Lightw. Europe 1, 31 (2002).
[1.8] P. J. Maguire, L. P. Barry T. Krug, W. H. Guo, J. O’Dowd, M. Lynch, A. L. Bradley, J. F. Donegan, and H. Folliot, “Optical signal processing via two-poton absorption in a semiconductor microcavity for the next generation of high-speed optical communications network,” J. Light. Technol. 24, 2683-2692 (2006).
[1.9] N. Suzuki, “FDTD analysis of two-photon absorption and free-carrier absorption in Si high-index-contrast waveguides,” J. Light. Technol. 25, 2495-2501 (2007).
[1.10] M. A. Foster, K. D. Moll, and A. L. Gaeta, “Optimal waveguide dimensions for nonlinear interactions,” Opt. Express 12, 2880-2887 (2004).
[1.11] K. K. Lee. D. R. Lim, A. Agarwal, D. Ripin, H. H. Fujimoto, M. Morse, and L. Kimerling, “Performance of polycrystalline silicon waveguide devices for compact on-chip optical interconnection,” Proc. SPIE 3847, 120-125 (1999).
[1.12] B. Miao, C. Chen, S. Shi, J. Murakowski, and D. W. Prather, “High-efficiency broad-band transmission through a boudle-60° bend in a planar photonic crystal single-line defect waveguide,” IEEE Photon. Technol. Lett. 16, 2469-2471 (2004).
[1.13] Y. Akahane, T. Asano, B.-S. Song, and S. Noda, “High-Q photonic nanocavity in a two-dimensional photonic crystal,” Nature 425, 944-947 (2003).
[1.14] P. Strasser, G. Stark, F. Robin, D. Erni, K. Rauscher, R. Wuest, and H. Jackel, “Optimization of a 60° waveguide bend in InP-based 2D planar photonic crystals,” J. Opt. Soc. Am. B 25, 67-73 (2008).
[1.15] S. H. Chang, T. C. Chiu, and C.-Y. Tai, “Propagation characteristics of the supermode based on two coupled semi-infinite rib plasmonic waveguides,” Opt. Express 15, 1755-1761 (2007).
[1.16] W. L. Barnes, A. Dereux, T. W. Ebbesen, “Surface plasmon subwavelength optics,” Nature 424, 824-830 (2003).
[1.17] S. I. Bozhevolnyi, V. S. Volkov, E. Devaux, and T. W. Ebbesen, “Channel plasmon-polariton guiding by subwavelength metal grooves,” Phys. Rev. Lett. 95,046802 (2005).
[1.18] S. I. Bozhevolnyi, V. S. Volkov, E. Devaux, J.-Y. Laluer, and T. W. Ebbesen, “Channel plasmon subwavelength waveguide components including interferometers and ring resonators,” Nature 440, 508-511 (2006).
[1.19] B. Wang and G. P. Wang, “Plasmon Bragg reflectors and nanocavities on flat metallic surfaces,” Appl. Phys. Lett. 87, 013107(2005).
[1.20] B. Wang and G. P. Wang, “Simulations of nanoscale interferometer and array focusing by metal heterowaveguides,” Opt. Express, 13, 10558-10563 (2005)
[1.21] X. Fan and G. P. Wang, “Nanoscale metal waveguide arrays as plasmon lenses,” Opt. Lett. 31, 1322-1324 (2006).
[1.22] H. Ditlbacher, J. R. Krenn, G. Schider, A. Leitner, and F. R. Aussenegg, “Two-dimensional optics with surface plasmon polaritons,” Appl. Phys. Lett. 81, 1762-1764 (2002).
[1.23] T. Goto, Y. Katagiri, H. Fukuda, H. Shinojima, Y. Nakano, I. Kobayashi, and Y. Mitsuoka, “Propagation loss measurement for surface plasmon-polariton modes at metal waveguides on semiconductor substrates,” Appl. Phys. Lett. 84, 852-854 (2004).
[1.24] J.-C. Weeber, M. U. Gonzalez, A.-L. Baudrion, and A. Dereux, “Surface plasmon routing along right angle bent metal strips,” Appl. Phys. Lett. 87, 221101 (2005).
[1.25] L. Chen, J. Shakya, and M. Lipson, “Subwavelength confinement in an integrated metal slot waveguide on silicon,” Opt. Lett. 15, 2133-2135 (2006).
[1.26] S. A. Maier, P. G. Kik, H. A. Atwater, S. Meltzer, E. Harel, B. E. Koel, and A. A. G. Requicha, “Local detection of electromagnetic energy transport below the diffraction limit in metal nanoparticle plasmon waveguides,” Nature material 12, 229-232 (2003).
[1.27] D. F. P. Pile and D. K. Gramotnev, “Channel plasmon-polariton in a triangular groove on a metal surface,” Opt. Lett. 29, 1069-1071 (2004).
[1.28] K. Tanaka, M. Tanaka, and T. Sugiyama, “Simulation of practical nanometric optical circuits based on surface plasmon polariton gap waveguides,” Opt. Express 13, 256-266 (2005).
[1.29] F. Kusunoki, T. Yotsuya, J. Takahara, and T. Kobayashi, “Propagation properties of guided waves in index-guided tw-dimensional optical waveguides,” Appl. Phys. Lett. 86, 211101 (2005).
[1.30] E. Moteno, F. J. Garcia-Vidal, S. G. Rodrigo, L. Martin-Moreno, and S. I. Bozhevolnyi, “Channel plasmon-polariton: modal shape, dispersion, and losses,” Opt. Lett. 31, 3447-3449 (2006).
[1.31] R. G. Hunsperger: Integrated Optics: Theory and Technology, 5th edn. (Springer, New York 2002) Chap. 3.
[1.32] I. V. Novikov and A. A. Maradudin, “Channel polaritions,” Phys. Rev. B 66, 035403 (2002).
[1.33] G. B. Hocker and W. K. Burns, “Mode dispersion in diffused channel waveguides by effective index method,” Appl. Opt. 16, 113-118 (1977).
[1.34] S. I. Bozhevolnyi and J. Jung, “Scaling for gap plasmon based waveguides,” Opt. Express 16, 2676-2684 (2008).
[1.35] F. Zheng, Z. Chen, and J. Zhang, “A finite-difference time-domain method without the Courant stability conditions,” IEEE Micro. Guided Wave Lett. 9, 441-443 (1999).
第二章
[2.1] R. W. Wood, “On a remarkable case of uneven distribution of light in a diffraction grating spectrum,” Proc. Phys. Soc. London 18, 269-275 (1902).
[2.2] U. Fano, “The theory of anomalous diffraction gratings and quasi-stationary waves on metallic surfaces (Sommerfeld’s waves),” J. Opt. Soc. Am. 32, 213-222 (1941).
[2.3] R. H. Ritchie, “Plasma losses by fast electrons in thin films,” Phys. Rev. 106, 874-881 (1957).
[2.4] E. A. Stern and R. A. Ferrell, “Surface plasma oscillations of a degenerate electron gas,” Phys. Rev. 120, 130-136 (1960).
[2.5] A. Otto, “Excitation of nonradiative surface plasma waves in silver by the method of frustrated total reflection,” Zeitschrift fur Physik 216, 398-410 (1968).
[2.6] R. F. Harrington: Time-Harmonic Electromagnetic Fields (John Wiley & Sons, New York 2001) Chap. 1.
[2.7] M. A. Ordal, Robert J. Bell, R. W. Alexander, Jr. L. L. Long, and M. R. Querry, “Optical properties of fourteen metals in the infrared and far infrared: Al, Co, Cu, Au, Fe, Pb, Mo, Ni, Pd, Pt, Ag, Ti, V and W,” Appl. Opt. 24, 4493-4499 (1985).
[2.8] H. Eherenreich and H. R. Philipp, “Optical properties of Ag and Cu,” Phys. Rev. 128, 1622-1629 (1962).
[2.9] H. Ehrenreich and H. R. Philipp, and B. Segall, “Optical properties of Aluminum,” Phys. Rev. 132, 1918-1928 (1963).
[2.10] A. D. Rakic, A. B. Djurisic, J. M. Elazar, and M. L. Majewski, “Optical properties of metallic films for vertical-cavity optoelectronic devices,” Appl. Opt. 37, 5271-5283 (1998).
[2.11] U. Kreibig and M. Vollmer: Optical Properties of Metal Clusters (Springer, New York 1995).
[2.12] E. Cottanich, G. Celep, J. Lerme, M. Pellarin, J. R. Huntzinger, J. L. Vialle, M. Broyer, “Optical properties of noble metal clusters as a function of the size: comparison between experiments and a semi-quantal theory,” Theor. Chem. Acc. 116, 514-523 (2006).
[2.13] H. G. Tompkins, S. Tasic, J. Baker, and D. Convey, “Spectroscopic ellipsometry measurements of thin metal films,” Surf. Interface Anal. 29, 179-187 (2000).
第三章
[3.1] A. Taflove, “Application of the finite-difference time-domain method to sinusoidal steady state electromagnetic penetration problems,” IEEE Trans. Electromag. Compat. 22, 191-202 (1980).
[3.2] K. S. Yee, “Numerical solution of initial boundary value problems involving Maxwell’s equations in isotropic media,” IEEE Trans. Antenna Propaga. 14, 302-307 (1966).
[3.3] R. Luebbers, F. P. Hunsberger, K. S. Kunz, R. B. Standler, and M. Schneider, “A frequency-dependent finite-difference time-domain formulation for dispersive materials,” IEEE Trans. Electromag. Compat. 32, 222-227 (1990).
[3.4] T. Kashiwa and I. Fukai, “A treatment by FDTD method of dispersive characteristics associated with electronic polarization,” Microwave Opt. Tech. Lett. 3, 203-205 (1990).
[3.5] D. M. Sullivan, “Frequency-dependent FDTD methods using Z transforms,” IEEE Trans. Antennas Propagat. 40, 1223-1230 (1992).
[3.6] W. C. Chew and W. H. Weedon, “A 3D perfectly matched medium from modified Maxwell’s equations with stretched coordinates,” Micro. Opt. Tech. Lett. 7, 599-604 (1994).
[3.7] G. Mur, “Absorbing boundary conditions for the finite-difference approximation of the time-domain electromagnetic-field equations,” IEEE Trans. Electromag. Compat. 23, 377-382 (1981).
[3.8] Z. P. Liao, H. L. Wong, B. P. Yang, and Y. F. Yuan, “A transmitting boundary for transient wave analysis,” Sci. Sin. Ser. A 27, 1063-1076 (1984).
[3.9] J. P. Berenger, “A perfectly matched layer for the absorption of electromagnetic waves,” J. Comput. Phys. 114, 185-200 (1994).
[3.10] A. P. Zhao, “Comments on “An efficient PML implementation for the ADI-FDTD method”,” IEEE Micro. Wire. Components Lett. 14, 248-249 (2000).
[3.11] G.-X. Fan, Q. H. Liu, “An FDTD Algorithm with perfectly matched layers for general dispersive media,” IEEE Trans. Antenna Propaga. 48, 637-646 (2000).
[3.12] G.-X. Fan, Q. H. Liu, and S. A. Hutchinson, “FDTD and PSTD simulations for plasma applications,” IEEE Trans. Plasma Sci. 29, 341-348 (2001).
[3.13] Q. H. Liu, “An FDTD algorithm with perfectly matched layers for conductive media,” Micro. Opt. Tech. Lett. 14, 134-137 (1997).
[3.14] R. W. Ziolkowski and J. B. Judkins, “ Full-wave vector Mwxwell equation modeling of the self-focusing of ultrashort optical pulses in a nonlinear Kerr medium exhibiting a finite response time,” J. Opt. Soc. Am. B 10, 186-198 (1993).
[3.15] R. W. Ziolkowski, “The incorporation of microscopic material models into the FDTD approach for ultrafast optical pulse simulations,” IEEE Trans. Antenna Propaga. 45, 375-391 (1997).
[3.16] M. Fujii, C. Koos, C. Poulton, I. Sakagami, J. Leuthold, and W. Freude, “A simple and rigorous verification technique for nonlinear FDTD algorithms by optical parametric four-wave mixing,” Micro. Opt. Tech. Lett. 48, 88-91 (2006).
[3.17] I. S. Maksymov, L. F. Marsal, J. Pallares, “Modeling of two-photon absorption in nonlinear photonic crystal all-optical switch,” Opt. Commun. 269, 137-141 (2007).
[3.18] R. A. Soref, and B. R. Bennett, “Electrooptical effects in Silicon,” IEEE Journal Quant. Elect. QE-23, 123-129 (1987).
[3.19] N. Suzuki, “FDTD analysis of two-photon absorption and free-carrier absorption in Si high-index-constrast waveguides,” J. Lightwave Tech. 25, 2495-2501 (2007).
[3.20] S. H. G. Teo, A. Q. Liu, J. B. Zhang, and M. H. Hong, “Induced free carrier modulation of photonic crystal optical intersection via localized optical absorption effect,” Appl. Phys. Lett. 89, 091910 (2006).
[3.21] T. K. Liang, L. R. Nunes, M. Tsuchiya, K. S. Abedin, T. Miyazaki, D. V. Thourhout, W. Bogaerts, P. Dumon, R. Baets, and H. K. Tsang, “High speed logic gate using two-photon absorption in silicon waveguides,” Opt. Commun. 265, 171-174 (2006).
第四章
[4.1] J. R. Krenn, B. Lamprecht, H. Ditlbacher, G. Schider, M. Salerno, A. Leitner, and F. R. Aussenegg, “Non-diffraction-limited light transport by gold nanowires,” Europhys. Lett. 60, 633 (2002).
[4.2] C. A. Pfeiffer, E. N. Economou, and K. L. Ngai, “Surface polaritons in a circularly cylindrical interface: surface plasmons,” Phy. Rev. B 10, 3038-3051 (1974).
[4.3] J. R. Krenn, A. Dereux, J. C. Webber, E. Bourillot, Y. Lacroute, J. P. Goudonnet, G. Schider, W. Gostschy, A. Leitner, F. R. Aussenegg, and C. Girard, “Squeezing the optical near-field zone by plasmon coupling of metallic nanoparticles,” Phy. Rev. Lett. 82, 2590-2593 (1999).
[4.4] K. Tananka, M. Tanaka, and T. Sugiyama, “Simulation of practical nanometeric optical circuits based on surface plasmon polariton gap waveguides,” Opt. Express 13, 256-266 (2005).
[4.5] D. F. Pile, T. Ogawa, D. K. Gramotnev, T. Okamoto, M. Haraguchi, M. Fukui, and S. Matsuo, “Theoretical and experimental investigation of strongly localized plasmons on triangular metal wedges for subwavelength waveguiding,” Appl. Phys. Lett. 87, 061106 (2005).
[4.6] S. I. Bozhevolnyi, V. S. Volkov, E. Deavux, and W. Ebbesen, “Channel plasmon-polariton guiding by subwavelength metal grooves,” Phys. Rev. Lett. 95, 046802 (2005).
[4.7] S. H. Chang, T. C. Chiu, and C.-Y. Tai, “Propagation characteristics of the supermode based on two coupled semi-infinite rib plasmonic waveguides,” Opt. Express 15, 1755-1761 (2007).
[4.8] S. H. Chang, C.-Y. Tai, T. C. Chiu, “The propagation characteristics of a dual channel directional coupler and a 90° bent waveguide based on coupled rib plasmonic waveguides,” Optics and Photonics, Taiwan, December 2006, BO-45 (2006).
[4.9] D. Dai, and Z. Sheng, “Numerical analysis of silicon-on-insulator ridge nanowires by using a full-vectorial finite-difference method mode solver,” J. Opt. Soc. Am. B 24, 2853-2859 (2007).
[4.10] C.-Y. Tai, S. H. Chang, T. C. Chiu, “Design and analysis of an ultra-compact and ultra-wideband polarization beam splitter based on coupled plasmonic waveguide arrays,” IEEE Photon. Techn. Lett. 19, 1448-1450 (2007).
[4.11] P. Wei, and W. Wang, “A TE-TM mode splitter on Lithium Niobate using Ti, Ni, ane MgO diffusions,” IEEE Photon. Technol. Lett. 6, 245-248 (1994).
[4.12] J. M. Hong, H. H. Ryu, S. R. Park, J. W. Jeong, S. G. Lee, E. H. Lee, S. G. Park, D. H. Woo, S. H. Kim, and B. H. O, “Design and fabrication of a significantly shortened multimode interference coupler for polarization splitter application,” IEEE Photon. Technol. Lett. 15, 72-74 (2003).
[4.13] L. B. Soldano, A. H. de Vreede, M. K. Smit, B. H. Verbeek, E. G. Metaal, and F. H. Groen, “Mach-Zehnder interferometer polarization splitter in InGaAsP-InP,” IEEE Photon. Technol. Lett. 6, 402-405(1994).
[4.14] W. N. Ye, D. X. Xu, S. Janz, P. Waldron, P. Cheben, and N. G. Tarr, “Passive broadband silicon-on-insulator polarization splitter,” Opt. Lett. 32, 1492-1494 (2007).
[4.15] C.-Y. Tai, S. H. Chang, and T. C. Chiu, “Optimization of wide-angle and broadband operational polarization beam splitter based on anisotropically coupled plasmonic waveguides array,” Accepted to be published in J. Opt. Soc. Am. B (2008).
[4.16] G. R. Bird and M. Parrish, “The wire grid as a near-infrared polarizer,” JOSA 50, 886-891 (1960).
[4.17] L. Zhou and W. Liu, “Broadband polarization beam splitter with and embedded metal-wire nanograting,” Opt. Lett. 30, 1434 (2005).
[4.18] H. J. Juretschke, “Comment on “Microscopic approach to reflection, transmission, and the Ewald-Ossen extinction theorem,” by Heidi Fearn, Daniel F. V. James, and Peter W. Milonni,” [Am. J. Phys. 64, 986-995], “ Am. J. Phys. 67, 929-930 (1999).
[4.19] H. A. Bethe, “Theory of diffraction by small holes,” Phys. Rev. 66, 163-182 (1944).
[4.20] S. I. Hosain, J. –P., Meunier, and Z. H. Wang, “Coupling efficiency of butt-joined planar waveguides with simultaneous tilt and transverse offset,” IEEE J. Lightwave Technol. 14, 901-907 (1996).
[4.21] Clifford R. Pollock and Michal Lipson, Integrated photonics. Boston:Kluwer Academic Publishers, 2003, pp.35-36.
[4.22] 李正中,薄膜光學與鍍膜技術第五版,藝軒圖書出版社(2006).
[4.23] X. Fan, G. P. Wang, Jeffrey C. W. Lee, C. T. Chan, “All-angle broadband negative refraction of metal waveguide arrays in the visible range: theoretical analysis and numerical demonstration,” Phys. Rev. Lett. 97, 073901 (2006).
[4.24] T. Liu, A. R. Zakharian, M. Fallahi, J. V. Moloney, and M. Mansuripur, “Design of a compact photonic-crystal-based polarizing beam splitter,” IEEE Photon. Technol. Lett. 17, 1435-1437 (2005).
[4.25] H. Fukuda, K. Yamada, T. Tai, T. Watanabe, H. Shinojima, and S. -I. Itabashi, “Ultrasmall polarization splitter based on silicon wire waveguides,” Opt. Express 14, 12401-12408 (2006).
[4.26] S. Kim, Gregory P. Nordin, J. Cai, and J. Jiang, “Ultracompact high-efficiency polarizing beam splitter with a hybrid photonic crystal and conventional waveguide structure,” Opt. Lett. 28, 2384-2386 (2003).
[4.27] X. Ao, L. Liu, L Wosinski, and S. He, “Polarization beam splitter based on a two-dimensional photonic crystal of pillar type,” Appl. Phys. Lett. 89, 171115 (2006).
[4.28] E. Hutter, J. Fendler, “Exploitation of Localized Surface Plasmon Resonance,” Adv. Mater. 16, 1685-1706 (2004).
[4.29] P. Tournios, Vincent Laude, “Negative group velocities in metal-film optical waveguides,” Opt. Commun. 137, 41-45 (1997).
[4.30] J. A. Dionne, L. A. Sweatlock, H. A. Atwater, A. Polman, “Planar metal plasmon waveguides: frequency-dependent dispersion, propagation, localization, and loss beyond the free electron model,” Phys. Rev. B 72, 075405 (2005).
[4.31] J. A. Dionne, L. A. Sweatlock, H. A. Atwater, A. Polman, “Plasmon slot waveguides: Towards chip-scale propagation with subwavelength-scale localization,” Phys. Rev. B 73, 035407 (2006).
[4.32] H. Shin and S. Fan, “All-angle negative refraction for surface plasmon waves using a metal-dielectric-metal structure,” Phys. Rev. Lett. 96, 073907 (2006).
[4.33] H. J. Lezec, J. A. Dionne, and H. A. Atwater, “Negative refraction at visible frequencies,” Science 316, 430-432 (2007).
[4.34] K. T. Wu, Y. D. Yao, W. B. Wu, and H. Z. Liu, “optical and magnetic studies in Ni-Ti alloy thin films,” in proceedings of 2003 Magnetics Conference, CS-14 (2003).
[4.35] C. Min, P. Wang, X. Jiao, Y. Deng, and H. Ming, “Beam manipulating by metallic nano-optics lens containing nonlinear media,” Opt. Express 15, 9541-9546 (2007).
[4.36] Q. Chen, L. Kuang, E. H. Sargent, and Z. Y. Wang, “Ultrafast nonresonant third-order optical nonlinearity of fullerene-containing polyurethane films at telecommunication wavelength, “Appl. Phys. Lett. 83, 2115-2117 (2003).
[4.37] H. Kosaka, T. Kawashima, A. Tomita, M. Notomi, T. Tamamura, T. Sato, and S. Kawakami, “Photonic crystals for micro lightwave circuits using wavelength-dependent angular beam steering,” Appl. Phys. Lett. 74, 1370-1372 (1999).
[4.38] G. S. He, L. Yuan, J. D. Bhawalkar, and P. N. Prasad, “Optical limiting, pulse reshaping, and stabilization with a nonlinear absorptive fiber system,” Appl. Opt. 36, 3387-3392 (1997).
[4.39] A. Nevejina-Srurhan, O. Werhahn, and U. Siegner, “Low-threshold high-dynamic-range optical limiter for ultra-short laser pulses,” Appl. Phys. B 74, 553-557 (2002).
[4.40] R. C. C. Leite, S. P. S. Porto, and T. C. Domen, “The thermal lens effects as power-limiting device,” Appl. Phys. Lett. 10, 100-101 (1967).
[4.41] K. M. Nashold, and D. P. Walter, “Investigation of optical limiting mechanisms in carbon particle suspensions and fullerene solutions,” J. Opt. Am. B 12, 1228-1237 (1995).
[4.42] D. Vincent, and J. Cruickshank, “Optical limiting with C60 and other fullerenes,” Appl. Opt. 36, 7794-7798 (1997).
[4.43] B. L. Justus, A. J. Campillo, A. L. Huston, “Thermal-defocusing /scattering optical limiter,” Opt. Lett. 19, 673-675 (1994).
[4.44] G. C. Duree, G. J. Salamo, M. Segev, A. Yariv, E. J. Sharp, and R. R. Neurgaonkar, “Photorefractive self-focusing and defocusing as an optical limiter,” Proc. SPIE 2229, 192-199 (1994).
[4.45] L. Porres, O. Mongin, C. Katan, M. Charlor, T. Pons, J. Mertz, and M. Balanchard-Desce, “Enhanced two-photon absorption with novel cutupolar propeller-shaped fluorophores derived from triphenylamine,” Org. Lett. 6, 47-50 (2004).
[4.46] O. Mongin, T. R. Krishna, M. H. V. Werts, A.-M. Caminade, J.-P. Majoral, and M. Blanchar-Desce, “A modular approach to two-photon absorption organic nanodots: brilliant dandrimers as alternative to semiconductor quamtum dots?,” Chem. Commun. , 915-917 (2006).
[4.47] S. Qu, Y. Gao, X. Jiang, H. Zeng, Y. Song, J. Qiu, C. Zhu, and K. Hirao, “Nonlinear absorption and optical limiting in gold-precipitated glasses induced by a femtosecond laser,” Opt. Commun. 224, 321-327 (2003).
[4.48] P. P. Kiran, B. N. S. Bhaktha, and D. N. Rao, “Nonlinear optical properties and surface plasmon enhanced optical limiting in Ag-Cu nanoclusters co-doped in SiO2 Sol-Gel films,” J. Appl. Phys. 96, 6717-6723 (2004).
[4.49] N. Izard, P. Billaud, D. Riehl, and E. Ahglaret, “Influence of structure on the optical limiting properties of nanotubes,” Opt. Lett. 30, 1509-1511 (2005).
[4.50] J.-B. Han, D.-J. Chen, S. Ding, H.-J. Zhou, Y.-B. Han, G.-G. Xiong, and Q.-Q. Wang, “Plasmon resonant absorption and third-order optical nonlinearity in Ag-Ti cosputtered composite films,” J. Appl. Phys. 99, 023526 (2006).
[4.51] H. Pan, W. Chen, Y. P. Feng, W. Ji, and J. Lin, “Optical limiting properties of metal nanowires,” Appl. Phys. Lett. 88, 223106 (2006).
[4.52] H. J. Elim, J. Yang, J.-Y. Lee, J. Mi, and W. Ji, “Observation of saturable and reverse-saturable absorption at longitudinal surface plasmon resonance in gold nanorods,” Appl. Phys. Lett. 88, 083107 (2006).
[4.53] S. Porel, N. Venkatram, D. N. Rao, T. P. Radhakrishnan, “Optical power limiting in the femtosecond regime by silver nanoparticle-embedded polymer film,” J. Appl. Phys. 102, 033107 (2007).
[4.54] T. K. Liang, L. R. Nunes, M. Tsuchiya, K. S. Abedin, T. Miyazaki, D. V. Thourhout, W. Bogaerts, P. Dumon, R. Baets, H. K. Tsang, “High speed logic gate using two-photon absorption in silicon waveguides,” Opt. Commun. 265, 171-174 (2006).
[4.55] M. Sheik-Bahae, D. J. Hagan, and E. W. V. Stryland, “Dispersion and band-gap scalling of the electronic kerr effect in solids associated with two-photon absorption,” Phys. Rev. Lett. 65, 96-99 (1990).
[4.56] M. Sheik-Bahae, D. C. Hurchings, D. J. Hagan, and E. W. V. Stryland, “Dispersion of band electronic nonlinear refraction in solids,” IEEE Quan. Electron. 27, 1296-1309 (1991).
[4.57] R. G. Hunsperger, Integrated Optics, 5th ed. (Springer, Berlin, 2002).
[4.58] N. Suzuki, “FDTD analysis of two-photon absorption and free-carrier absorption in Si high-index-constrast waveguides,” J. Lightwave Tech. 25, 2495-2501 (2007).
[4.59] Q. Xu and M. Lipson, “All-optical logic based on silicon micro-ring resonators,” Opt. Express 15, 924-929 (2007).
[4.60] S. Manipatruni, Q. Xu, B. Schmidt, J. Shakya, and M. Lipson, “High speed carrier injection 18Gb/s Silicon micro-ring electro-optic modulator,” LEOS 2007, 21-25 (2007).
[4.61] K. Preston, P. Dong, Bradley Schmidt, and M. Lipson, “High-speed all-optical modulation using polycrystalline silicon microring resonators,” Appl. Phys. Lett. 92, 151104 (2008).
[4.62] C. Kittle, Introduction to Solid State Physics, 7th ed. (John Wiely & Sons, 1996).
[4.63] S. Gupta, M. Y. Frankel, J. A. Valdmanis, J. F. Whitaker, and G. A. Mourou, “Subpicosecond carrier lifetime in GaAs grown by molecular beam epitaxy at low temperatures,” Appl. Phys. Lett. 59, 3276-3278 (1991). |