1.Department of Physics and Center for Applied Photonics, University of Konstanz, 78457, Konstanz, Germany
2.School of Engineering, University of Glasgow, Rankine Building, Oakfield Avenue, Glasgow, G12 8LT, UK
3.L-NESS, Dipartimento di Fisica del Politecnico di Milano, Via Anzani 42, 22100, Como, Italy
4.Dipartimento di Fisica, Politecnico di Milano, Piazza Leonardo da Vinci 32, 20133, Milano, Italy
5.Department of Physics, Sapienza University of Rome, 00185, Rome, Italy
6.Physics and Materials Science Research Unit, University of Luxembourg, 162a avenue de la Faïencerie, L-1511, Luxembourg, Luxembourg
Daniele Brida (daniele.brida@uni.lu)
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Marco P. Fischer, Aaron Riede, Kevin Gallacher, 等. Plasmonic mid-infrared third harmonic generation in germanium nanoantennas[J]. 光:科学与应用, 2018,7(6):1001-1007.
Fischer, M. P. et al. Plasmonic mid-infrared third harmonic generation in germanium nanoantennas. Light: Science & Applications, 7, 1001-1007 (2018).
Marco P. Fischer, Aaron Riede, Kevin Gallacher, 等. Plasmonic mid-infrared third harmonic generation in germanium nanoantennas[J]. 光:科学与应用, 2018,7(6):1001-1007. DOI: 10.1038/s41377-018-0108-8.
Fischer, M. P. et al. Plasmonic mid-infrared third harmonic generation in germanium nanoantennas. Light: Science & Applications, 7, 1001-1007 (2018). DOI: 10.1038/s41377-018-0108-8.
We demonstrate third harmonic generation in plasmonic antennas consisting of highly doped germanium grown on silicon substrates and designed to be resonant in the mid-infrared frequency range that is inaccessible with conventional nonlinear plasmonic materials. Owing to the near-field enhancement, the result is an ultrafast, subdiffraction, coherent light source with a wavelength tunable between 3 and 5 µm, and ideally overlapping with the fingerprint region of molecular vibrations. To observe the nonlinearity in this challenging spectral window, a high-power femtosecond laser system equipped with parametric frequency conversion in combination with an all-reflective confocal microscope setup is employed. We demonstrate spatially resolved maps of the linear scattering cross section and the nonlinear emission of single isolated antenna structures. A clear third-order power dependence as well as mid-infrared emission spectra prove the nonlinear nature of the light emission. Simulations support the observed resonance length of the double-rod antenna and demonstrate that the field enhancement inside the antenna material is responsible for the nonlinear frequency mixing.
Novotny, L. & Van Hulst, N. Antennas for light. Nat. Photonics 5, 83–90 (2011).
Biagioni, P., Huang, J. S. & Hecht, B. Nanoantennas for visible and infrared radiation. Rep. Prog. Phys. 75, 024402 (2012).
Kauranen, M. & Zayats, A. V. Nonlinear plasmonics. Nat. Photonics 6, 737–748 (2012).
Hanke, T. et al. Efficient nonlinear light emission of single gold optical antennas driven by few-cycle near-infrared pulses. Phys. Rev. Lett. 103, 257404 (2009).
Vampa, G. et al. Plasmon-enhanced high-harmonic generation from silicon. Nat. Phys. 13, 659–662 (2017).
Lee, J. et al. Giant nonlinear response from plasmonic metasurfaces coupled to intersubband transitions. Nature 511, 65–69 (2014).
Razdolski, I. et al. Resonant enhancement of second-harmonic generation in the mid-infrared using localized surface phonon polaritons in subdiffractional nanostructures. Nano Lett. 16, 6954–6959 (2016).
Hafez, H. A. et al. Extremely efficient terahertz high-harmonic generation in graphene by hot Dirac fermions. Nature 561, 507–511 (2018).
Guo, H. R. et al. Mid-infrared frequency comb via coherent dispersive wave generation in silicon nitride nanophotonic waveguides. Nat. Photonics 12, 330–335 (2018).
Chang, Y. C. et al. Realization of mid-infrared graphene hyperbolic metamaterials. Nat. Commun. 7, 10568 (2016).
Law, S., Yu, L., Rosenberg, A. & Wasserman, D. All-semiconductor plasmonic nanoantennas for infrared sensing. Nano Lett. 13, 4569–4574 (2013).
Guilengui, V. N., Cerutti, L., Rodriguez, J. B., Tournié, E. & Taliercio, T. Localized surface plasmon resonances in highly doped semiconductors nanostructures. Appl. Phys. Lett. 101, 161113 (2012).
Panah, M. E. A. et al. Mid-IR optical properties of silicon doped InP. Opt. Mater. Express 7, 2260–2271 (2017).
Soref, R. Mid-infrared photonics in silicon and germanium. Nat. Photonics 4, 495–497 (2010).
Baldassarre, L. et al. Midinfrared plasmon-enhanced spectroscopy with germanium antennas on silicon substrates. Nano Lett. 15, 7225–7231 (2015).
Frigerio, J. et al. Tunability of the dielectric function of heavily doped germanium thin films for mid-infrared plasmonics. Phys. Rev. B 94, 085202 (2016).
Neubrech, F. et al. Resonant plasmonic and vibrational coupling in a tailored nanoantenna for infrared detection. Phys. Rev. Lett. 101, 157403 (2008).
Adato, R. et al. Ultra-sensitive vibrational spectroscopy of protein monolayers with plasmonic nanoantenna arrays. Proc. Natl Acad. Sci. USA 106, 19227–19232 (2009).
Brown, L. V. et al. Surface-enhanced infrared absorption using individual cross antennas tailored to chemical moieties.J. Am. Chem. Soc. 135, 3688–3695 (2013).
Strikwerda, A. C., Zalkovskij, M., Iwaszczuk, K., Lorenzen, D. L. & Jepsen, P. U. Permanently reconfigured metamaterials due to terahertz induced mass transfer of gold. Opt. Express 23, 11586–11599 (2015).
Hon, N. K., Soref, R. & Jalali, B. The third-order nonlinear optical coefficients of Si, Ge, and Si 1-xGex in the midwave and longwave infrared. J. Appl. Phys. 110, 011301 (2011).
Zhang, L., Agarwal, A. M., Kimerling, L. C. & Michel, J. Nonlinear group Ⅳ photonics based on silicon and germanium: from near-infrared to mid-infrared. Nanophotonics 3, 247–268 (2014).
Boyd, R. W., Shi, Z. M. & De Leon, I. The third-order nonlinear optical susceptibility of gold. Opt. Commun. 326, 74–79 (2014).
Fischer, M. P. et al. Optical activation of germanium plasmonic antennas in the mid-infrared. Phys. Rev. Lett. 117, 047401 (2016).
Mesch, M., Metzger, B., Hentschel, M. & Giessen, H. Nonlinear plasmonic sensing. Nano Lett. 16, 3155–3159 (2016).
Höppener, C. & Novotny, L. Imaging of membrane proteins using antenna-based optical microscopy. Nanotechnology 19, 384012 (2008).
Palomba, S. & Novotny, L. Near-field imaging with a localized nonlinear light source. Nano Lett. 9, 3801–3804 (2009).
Ginzburg, P., Krasavin, A. V., Wurtz, G. A. & Zayats, A. V. Nonperturbative hydrodynamic model for multiple harmonics generation in metallic nanostructures. ACS Photonics 2, 8–13 (2015).
Sakat, E. et al. Near-field imaging of free carriers in ZnO nanowires with a scanning probe tip made of heavily doped germanium. Phys. Rev. Appl. 8, 054042 (2017).
Rosenblad, C. et al. Silicon epitaxy by low-energy plasma enhanced chemical vapor deposition. J. Vac. Sci. Technol. A 16, 2785–2790 (1998).
Frigerio, J. et al. Optical properties of highly n-doped germanium obtained by in situ doping and laser annealing. J. Phys. D. Appl. Phys. 50, 465103 (2017).
Paul D. J. et al. n-Ge on Si for mid-infrared plasmonic sensors. In Proc. of 2017 IEEE Photonics Society Summer Topical Meeting Series 125–126 (IEEE, San Juan, Puerto Rico, 2017). https://doi.org/10.1109/PHOSST.2017.8012682https://doi.org/10.1109/PHOSST.2017.8012682
Mirza, M. M. et al. Nanofabrication of high aspect ratio (~50:1) sub-10 nm silicon nanowires using inductively coupled plasma etching. J. Vac. Sci. Technol. B 30, 06FF02 (2012).
Grupp, A. et al. Broadly tunable ultrafast pump-probe system operating at multi-kHz repetition rate. J. Opt. 20, 014005 (2018).
Antipenkov, R., Varanavičius, A., Zaukevičius, A. & Piskarskas, A. P. Femtosecond Yb:KGW MOPA driven broadband NOPA as a frontend for TW few-cycle pulse systems. Opt. Express 19, 3519–3524 (2011).
Junginger, F. et al. Single-cycle multiterahertz transients with peak fields above 10 MV/cm. Opt. Lett. 35, 2645–2647 (2010).
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