Nonlinear chiral imaging of subwavelength-sized twisted-cross gold nanodimers [Invited]
نویسندگان
چکیده
We perform second-harmonic generation (SHG) microscopy with circularly polarized (CP) light to measure chirality of individual twistedcross gold nanodimers. The chiral signatures, based on different SHG response for the two CP components of incident light, are clearly visible even with off-resonance excitation. The SHG responses of individual nanodimers are found to vary by about a factor of five. The technique thus has very high sensitivity to the nanoscale deformations of the structure. The chiral signatures of the dimers, however, are found to be more uniform, and the technique is thus able to recognize the handedness of the twisted nanodimers with high reliability. ©2011 Optical Society of America OCIS codes: (180.4315) Nonlinear microscopy; (190.4350) Nonlinear optics at surfaces; (160.1585) Chiral media; (160.3918) Metamaterials. References and links 1. L. D. Barron, Molecular Light Scattering and Optical Activity (Cambridge University Press, 1982). 2. V. M. Shalaev, “Optical negative-index metamaterials,” Nat. Photonics 1(1), 41–48 (2007). 3. C. M. Soukoulis, S. Linden, and M. Wegener, “Negative refractive index at optical wavelengths,” Science 315(5808), 47–49 (2007). 4. A. S. Schwanecke, A. Krasavin, D. M. Bagnall, A. Potts, A. V. Zayats, and N. I. Zheludev, “Broken time reversal of light interaction with planar chiral nanostructures,” Phys. Rev. Lett. 91(24), 247404 (2003). 5. S. Tretyakov, I. Nefedov, A. Sihvola, S. Maslovski, and C. Simovski, “Waves and energy in chiral nihility,” J. Electromagn. Waves Appl. 17(5), 695–706 (2003). 6. J. B. Pendry, “A chiral route to negative refraction,” Science 306(5700), 1353–1355 (2004). 7. E. Plum, J. Zhou, J. Dong, V. A. Fedotov, T. Koschny, C. M. Soukoulis, and N. I. Zheludev, “Metamaterial with negative index due to chirality,” Phys. Rev. B 79(3), 035407 (2009). 8. S. Zhang, Y.-S. Park, J. Li, X. Lu, W. Zhang, and X. Zhang, “Negative refractive index in chiral metamaterials,” Phys. Rev. Lett. 102(2), 023901 (2009). 9. M. Kuwata-Gonokami, N. Saito, Y. Ino, M. Kauranen, K. Jefimovs, T. Vallius, J. Turunen, and Y. Svirko, “Giant optical activity in quasi-two-dimensional planar nanostructures,” Phys. Rev. Lett. 95(22), 227401 (2005). 10. M. Decker, M. W. Klein, M. Wegener, and S. Linden, “Circular dichroism of planar chiral magnetic metamaterials,” Opt. Lett. 32(7), 856–858 (2007). 11. A. V. Rogacheva, V. A. Fedotov, A. S. Schwanecke, and N. I. Zheludev, “Giant gyrotropy due to electromagnetic-field coupling in a bilayered chiral structure,” Phys. Rev. Lett. 97(17), 177401 (2006). 12. E. Plum, V. A. Fedotov, A. S. Schwanecke, N. I. Zheludev, and Y. Chen, “Giant optical gyrotropy due to electromagnetic coupling,” Appl. Phys. Lett. 90(22), 223113 (2007). 13. J. K. Gansel, M. Thiel, M. S. Rill, M. Decker, K. Bade, V. Saile, G. von Freymann, S. Linden, and M. Wegener, “Gold helix photonic metamaterial as broadband circular polarizer,” Science 325(5947), 1513–1515 (2009). 14. M. Thiel, M. S. Rill, G. von Freymann, and M. Wegener, “Three-dimensional bi-chiral photonic crystals,” Adv. Mater. (Deerfield Beach Fla.) 21(46), 4680–4682 (2009). 15. M. Decker, M. Ruther, C. E. Kriegler, J. Zhou, C. M. Soukoulis, S. Linden, and M. Wegener, “Strong optical activity from twisted-cross photonic metamaterials,” Opt. Lett. 34(16), 2501–2503 (2009). 16. M. Decker, R. Zhao, C. M. Soukoulis, S. Linden, and M. Wegener, “Twisted split-ring-resonator photonic metamaterial with huge optical activity,” Opt. Lett. 35(10), 1593–1595 (2010). #142344 $15.00 USD Received 7 Feb 2011; revised 4 Mar 2011; accepted 4 Mar 2011; published 22 Apr 2011 (C) 2011 OSA 1 May 2011 / Vol. 1, No. 1 / OPTICAL MATERIALS EXPRESS 46 17. M. I. Stockman, D. J. Bergman, C. Anceau, S. Brasselet, and J. Zyss, “Enhanced second-harmonic generation by metal surfaces with nanoscale roughness: nanoscale dephasing, depolarization, and correlations,” Phys. Rev. Lett. 92(5), 057402 (2004). 18. M. W. Klein, C. Enkrich, M. Wegener, and S. Linden, “Second-harmonic generation from magnetic metamaterials,” Science 313(5786), 502–504 (2006). 19. M. W. Klein, M. Wegener, N. Feth, and S. Linden, “Experiments on secondand third-harmonic generation from magnetic metamaterials,” Opt. Express 15(8), 5238–5247 (2007). 20. N. Feth, S. Linden, M. W. Klein, M. Decker, F. B. P. Niesler, Y. Zeng, W. Hoyer, J. Liu, S. W. Koch, J. V. Moloney, and M. Wegener, “Second-harmonic generation from complementary split-ring resonators,” Opt. Lett. 33(17), 1975–1977 (2008). 21. F. B. P. Niesler, N. Feth, S. Linden, J. Niegemann, J. Gieseler, K. Busch, and M. Wegener, “Second-harmonic generation from split-ring resonators on a GaAs substrate,” Opt. Lett. 34(13), 1997–1999 (2009). 22. B. K. Canfield, H. Husu, J. Laukkanen, B. Bai, M. Kuittinen, J. Turunen, and M. Kauranen, “Local field asymmetry drives second-harmonic generation in non-centrosymmetric nanodimers,” Nano Lett. 7(5), 1251– 1255 (2007). 23. H. Tuovinen, M. Kauranen, K. Jefimovs, P. Vahimaa, T. Vallius, J. Turunen, N. V. Tkachenko, and H. Lemmetyinen, “Linear and second-order nonlinear optical properties of arrays of noncentrosymmetric gold nanoparticles,” J. Nonlinear Opt. Phys. Mater. 11(4), 421–432 (2002). 24. B. K. Canfield, S. Kujala, K. Jefimovs, J. Turunen, and M. Kauranen, “Linear and nonlinear optical responses influenced by broken symmetry in an array of gold nanoparticles,” Opt. Express 12(22), 5418–5423 (2004). 25. B. K. Canfield, H. Husu, J. Kontio, J. Viheriala, T. Rytkonen, T. Niemi, E. Chandler, A. Hrin, J. A. Squier, and M. Kauranen, “Inhomogeneities in the nonlinear tensorial responses of arrays of gold nanodots,” N. J. Phys. 10(1), 013001 (2008). 26. B. K. Canfield, S. Kujala, K. Laiho, K. Jefimovs, J. Turunen, and M. Kauranen, “Chirality arising from small defects in gold nanoparticle arrays,” Opt. Express 14(2), 950–955 (2006). 27. S. Kujala, B. K. Canfield, M. Kauranen, Y. Svirko, and J. Turunen, “Multipole interference in the secondharmonic optical radiation from gold nanoparticles,” Phys. Rev. Lett. 98(16), 167403 (2007). 28. H. Husu, B. K. Canfield, J. Laukkanen, B. Bai, M. Kuittinen, J. Turunen, and M. Kauranen, “Chiral coupling in gold nanodimers,” Appl. Phys. Lett. 93(18), 183115 (2008). 29. P. M. Rentzepis, J. A. Giordmaine, and K. W. Wecht, “Coherent optical mixing in optically active liquids,” Phys. Rev. Lett. 16(18), 792–794 (1966). 30. A. P. Shkurinov, A. V. Dubrovskii, and N. I. Koroteev, “Second harmonic generation in an optically active liquid: Experimental observation of a fourth-order optical nonlinearity due to molecular chirality,” Phys. Rev. Lett. 70(8), 1085–1088 (1993). 31. P. Fischer, D. S. Wiersma, R. Righini, B. Champagne, and A. D. Buckingham, “Three-wave mixing in chiral liquids,” Phys. Rev. Lett. 85(20), 4253–4256 (2000). 32. M. A. Belkin, T. A. Kulakov, K.-H. Ernst, L. Yan, and Y. R. Shen, “Sum-frequency vibrational spectroscopy on chiral liquids: a novel technique to probe molecular chirality,” Phys. Rev. Lett. 85(21), 4474–4477 (2000). 33. M. Kauranen, T. Verbiest, and A. Persoons, “Second-order nonlinear optical signatures of surface chirality,” J. Mod. Opt. 45(2), 403–423 (1998). 34. J. Hicks, Chirality: Physical Chemistry, ACS Symposium Series 810 (American Chemical Society, 2002). 35. S. Sioncke, T. Verbiest, and A. Persoons, “Second-order nonlinear optical properties of chiral materials,” Mater. Sci. Eng. Rep. 42(5-6), 115–155 (2003). 36. M. A. Belkin and Y. R. Shen, “Non-linear optical spectroscopy as a novel probe for molecular chirality,” Int. Rev. Phys. Chem. 24(2), 257–299 (2005). 37. T. Verbiest, M. Kauranen, Y. Van Rompaey, and A. Persoons, “Optical activity of anisotropic achiral surfaces,” Phys. Rev. Lett. 77(8), 1456–1459 (1996). 38. M. Siltanen, E. Vuorimaa, H. Lemmetyinen, P. Ihalainen, J. Peltonen, and M. Kauranen, “Nonlinear optical and structural properties of langmuir-blodgett films of thiohelicenebisquinones,” J. Phys. Chem. B 112(7), 1940– 1945 (2008). 39. V. A. Makarov and I. A. Perezhogin, “Generation of reflected second-harmonic light beam with inhomogeneous transversal distribution of polarization from the surface of chiral medium by normally incident Gaussian beam,” Opt. Commun. 281(14), 3906–3912 (2008). 40. M. J. Huttunen, M. Erkintalo, and M. Kauranen, “Absolute nonlinear optical probes of surface chirality,” J. Opt. A, Pure Appl. Opt. 11(3), 034006 (2009). 41. M. J. Huttunen, M. Virkki, M. Erkintalo, E. Vuorimaa, A. Efimov, H. Lemmetyinen, and M. Kauranen, “Absolute probe of surface chirality based on focused circularly polarized light,” J. Phys. Chem. Lett. 1(12), 1826–1829 (2010). 42. T. Petralli-Mallow, T. M. Wong, J. D. Byers, H. I. Yee, and J. M. Hicks, “Circular dichroism spectroscopy at interfaces: A surface second harmonic generation study,” J. Phys. Chem. 97(7), 1383–1388 (1993). 43. J. D. Byers, H. I. Yee, and J. M. Hicks, “A second harmonic generation analog of optical rotator dispersion for the study of chiral monolayers,” J. Chem. Phys. 101(7), 6233–6241 (1994). 44. J. D. Byers, H. I. Yee, T. Petralli-Mallow, and J. M. Hicks, “Second-harmonic generation circular-dichroism spectroscopy from chiral monolayers,” Phys. Rev. B Condens. Matter 49(20), 14643–14647 (1994). #142344 $15.00 USD Received 7 Feb 2011; revised 4 Mar 2011; accepted 4 Mar 2011; published 22 Apr 2011 (C) 2011 OSA 1 May 2011 / Vol. 1, No. 1 / OPTICAL MATERIALS EXPRESS 47 45. M. Kauranen, T. Verbiest, J. J. Maki, and A. Persoons, “Second-harmonic generation from chiral surfaces,” J. Chem. Phys. 101(9), 8193–8199 (1994). 46. T. Verbiest, M. Kauranen, J. J. Maki, M. N. Teerenstra, A. J. Schouten, R. J. M. Nolte, and A. Persoons, “Linearly polarized probes of surface chirality,” J. Chem. Phys. 103(18), 8296–8298 (1995). 47. J. J. Maki, T. Verbiest, M. Kauranen, S. V. Elshocht, and A. Persoons, “Comparison of linearly and circularly polarized probes of second-order optical activity of chiral surfaces,” J. Chem. Phys. 105(2), 767–772 (1996). 48. M. C. Schanne-Klein, F. Hache, A. Roy, C. Flytzanis, and C. Payrastre, “Off resonance second order optical activity of isotropic layers of chiral molecules: Observation of electric and magnetic contributions,” J. Chem. Phys. 108(22), 9436–9443 (1998). 49. G. J. Simpson, “Molecular origins of the remarkable chiral sensitivity of second-order nonlinear optics,” ChemPhysChem 5(9), 1301–1310 (2004). 50. S. A. Mitchell and R. A. McAloney, “Second harmonic optical activity of tryptophan derivatives adsorbed at the air/water interface,” J. Phys. Chem. B 108(3), 1020–1029 (2004). 51. M. A. Kriech and J. C. Conboy, “Counterpropagating second-harmonic generation: A new technique for the investigation of molecular chirality at surfaces,” J. Opt. Soc. Am. B 21(5), 1013–1022 (2004). 52. M. A. Kriech and J. C. Conboy, “Imaging chirality with surface second harmonic generation microscopy,” J. Am. Chem. Soc. 127(9), 2834–2835 (2005). 53. N. Ji, K. Zhang, H. Yang, and Y. R. Shen, “Three-dimensional chiral imaging by sum-frequency generation,” J. Am. Chem. Soc. 128(11), 3482–3483 (2006). 54. G. Subramania and S. Y. Lin, “Fabrication of three-dimensional photonic crystal with alignment based on electron beam lithography,” Appl. Phys. Lett. 85(21), 5037–5039 (2004). 55. N. Liu, H. Liu, S. Zhu, and H. Giessen, “Stereometamaterials,” Nat. Photonics 3(3), 157–162 (2009). 56. V. K. Valev, N. Smisdom, A. V. Silhanek, B. De Clercq, W. Gillijns, M. Ameloot, V. V. Moshchalkov, and T. Verbiest, “Plasmonic ratchet wheels: switching circular dichroism by arranging chiral nanostructures,” Nano Lett. 9(11), 3945–3948 (2009). 57. V. K. Valev, A. V. Silhanek, N. Smisdom, B. De Clercq, W. Gillijns, O. A. Aktsipetrov, M. Ameloot, V. V. Moshchalkov, and T. Verbiest, “Linearly polarized second harmonic generation microscopy reveals chirality,” Opt. Express 18(8), 8286–8293 (2010). 58. V. K. Valev, A. V. Silhanek, N. Verellen, W. Gillijns, P. Van Dorpe, O. A. Aktsipetrov, G. A. Vandenbosch, V. V. Moshchalkov, and T. Verbiest, “Asymmetric optical second-harmonic generation from chiral G-shaped gold nanostructures,” Phys. Rev. Lett. 104(12), 127401 (2010).
منابع مشابه
Optical Chirality Enhancement in Twisted Arrays of Plasmonic Nano-rods
An important property of electromagnetic fields, which arises from the interaction between fields and chiral molecules, is called optical chirality. By enhancing this field property, while maintaining constant input power, we are able to increase absorption of circularly polarized light by chiral molecules of a certain handedness. This enhancement is achieved through the use of achiral plasmoni...
متن کاملDependence of resonant light transmission properties of a subwavelength slit on structural parameters.
We perform a systematic study of the resonant transmission of visible and near-infrared (NIR) light through a single subwavelength slit in a gold film when the parameters defining the structure are varied. We further examine the optical properties of a related nanostructure, a cross with subwavelength sized features. Focused ion beam (FIB) milling was used to fabricate nanoslits and crosses wit...
متن کاملVisible quantum plasmonics from metallic nanodimers
We report theoretical evidence that bulk nonlinear materials weakly interacting with highly localized plasmonic modes in ultra-sub-wavelength metallic nanostructures can lead to nonlinear effects at the single plasmon level in the visible range. In particular, the two-plasmon interaction energy in such systems is numerically estimated to be comparable with the typical plasmon linewidths. Locali...
متن کاملHighly asymmetric transmission of linearly polarized waves realized with a multilayered structure including chiral metamaterials
We numerically and experimentally demonstrate highly asymmetric transmission of linearly polarized waves with a multilayered metallic structure. The whole structure has a subwavelength thickness and consists of a thin slab of chiral metamaterial sandwiched between two 90◦ twisted linear polarizers. The chiral metamaterial is made of two sets of twisting cross wires that can rotate the polarizat...
متن کاملChiral meta-atoms rotated by light
We study the opto-mechanical properties of coupled chiral meta-atoms based on a pair of twisted split-ring resonators. By using a simple analytical model in conjunction with the Maxwell stress tensor, we capture insight into the mechanism and find that this structure can be used as a general prototype of subwavelength light-driven actuators over a wide range of frequencies. This coupled structu...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2011