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Qihuang Gong, Xiaoyong Hu, Jiaxiang Zhang, Hong Yang Department of Physics, Peking University, Beijing, P. R. China Composite Materials for Ultrafast and Large Third-order Optical Nonlinearity and Photonic Applications Email: qhgong@pku.edu.cn; Fax: +86-10-62756567qhgong@pku.edu.cn
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Contents Motivation Enhanced ultrafast 3rd nonlinearity using composite materials Photonic crystal and PC optical switch Conclusion
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I.Motivation 1980- Third-order Optical Nonlinear Materials Photonics Applications Fast and large 3 rd NLO response fs NLO response large off-resonant (3) All optical device Optical switching Optical computing conjugated organic molecules and polymers Semiconductors } fs measur. Integrated photonic circuits
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Femtosecond OKE System : 760 - 850nm : ~ 100fs I 1 :I 2 = 10:1 Measurement on ultrafast 3 rd nonlinearity
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E1E1 E2E2 EsEs IsIs I1I1 I2I2 (3) E2E2 E1E1 EsEs 45 0 Is =Is = P Typical OKE signal of CS 2 OKE – four wave mixing process
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3 rd optical nonlinearity of routine materials : NLO materials n 2 (m 2 /W) t(s) Organic polymers 10 -16 -10 -17 10 -15 Semiconductor 10 -17 10 -13 ☆ Large 3 rd nonlinear susceptibility and ultrafast response are difficult to achieve simultaneously Liquid crystal 10 -7 10 -6
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Composite I: Coumarine 153 doped Polystyrene * Inter-molecular excited-state electron transfer II Enhanced ultrafast 3 rd nonlinearity using composite materials n 2 ( (3) ) ~ 1/( 0 – – i ) * Near resonant enhancement (enlarge the response time of excited state lifetime )
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800nm probe Inter molecular electron transfer C153 molecule ~ 1ps Coumarine 153 doped Polystyrene Polystyrene 400nm near-resonant excitation Polymer composite material: C153:Polystyrene
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The effective third-order nonlinear optical susceptibility of the composite material can be written as and are permittivity for host material and metal nanoparticles and are third-order optical susceptibility of host material and metal nanoparticles In the SPR peak a very large nonlinear coefficient p is the volume fraction of Ag nanoparticles Composite Material II: Nano-Ag doped MEH-PPV surface plasmonics enhanced 3 rd optical nonlinearity
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Nano-Ag doped MEH-PPV Ag nanoparticle Energy transfer ~ ps MEH-PPV SPR resonant excitation
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★ Photonic crystal is a novel photonic material with a One-dimensional Photonic crystal Two-dimensional photonic crystal Three-dimensional photonic crystal ★ Photonic crystal possesses photonic bandgap and periodic dielectric distribution can control the propagation states of photons III. Photonic crystal and PC optical switch
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Defect Radius Dielectric Defect Frequency Air Defect Air Band Dielectric Band Defect states When a structure defect is introduced in the photonic crystal, the defect states will appear in the photonic bandgap Photonic Bnadgap
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Photonic Bandgap Shift ☆ Third-order optical nonlinear photonic crystal Bandgap or Defect state shift ---------- change the refractive index Probe LightPump Light Wavelength Transmittance Photonic Bandgap Pump LightProbe Light Transmittance Wavelength Defect State Photonic Bandgap Defect State Shift Pump Beam Intensity Light beam controlled Shift
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Concept for All-Optical Switching effect Probe light Pump light Using Photonic bandgap shift or defect state shift by Pump Beam Photonic crystal optical switching Probe light
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Schematic Structure of Polystyrene Molecule Organic polymer: Polystyrene n 2 = 1×10 -13 cm 2 /W 1) PC optical switch using pure polymer
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Film Thickness 300nm Lattice Constant 320nm Radius of Air Hole 130nm Width of Line Defect 450nm Two-dimensional Polystyrene Photonic Crystal Fabrication Process A line defect in the center of a two- dimensional photonic crystal to form photonic crystal filter Spin Coating + FIB etching cylindrical air holes embodied in the polystyrene slab. The patterned area is about 4 μm×100 μm
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Transmission spectra : (a) Measured result (b) Theoretical result of multiple scattering method Photonic Crystal Devices: Filter, Switch line defect transmission mode * Central Wavelength 791nm, Quality Factor 500, Line width 1.6nm
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Evanescent Field Coupling System 2) Coupling efficiency ~ 20% 1) Energy of the incident light is coupled into optical waveguide with the help of evanescent field Cross Section StructureElectric-field Distribution W θpθp Waveguide Substrate Air Gap Substrate Waveguide Prism Mode Guided Mode Air Gap X Z probe beam
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Experimental Setup Ti:sapphire laser: Pulse Duration 120fs Pulse Repetition 76MHz Wavelength 700nm - 860nm PMT Computer Monochromator Prism LensAperture Ti:sapphire Laser Diode Delay Line Micro Lens Waveguide 100 μm×2.5 mm The patterned area is about 4 μm×100 μm 800nm Pump beam 800nm
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Time Response ( as fast as the time- resolution of measurement system ) Conclusion: An all-polymer tunable photonic crystal filter, switch with ultrafast time response is realized. * Transmittance Contrast 60 % * Time Response ~ 120fs Pump Intensity as high as GW/cm 2 800nm Pump beam Switching Performance
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2) C153:Polystyrene PC optical switch Lattice constant: 320nm Air hole radius: 120nm Film thichness: 300nm Line defect width: 440nm Polystyrene doped with 15% Coumarin 153 Absorption peak of Coumarin 153 is around 400nm
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Electric field distribution of defect mode Electric field was mainly confined in the defect structure
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Measured result Simulated result Transmittance spectra of the microcavity resonant mode as functions of the energy of the pump light Tunability of the photonic bandgap microcavity
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Experimental setup Ti:sapphire Laser PMT Computer Fiber Spectrophotometer Prism LensAperture Delay Line Micro Lens BBO Crystal Filter Near-resonant enhanced ----- 400nm Pump beam ☆ Near-resonant enhanced nonlinearity of polystyrene 400nm 800nm
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Response time: 1.2ps All-optical switch effect Switching efficiency: 80% Pump power: 110 KW/cm 2 (reduced by 4 orders) Nature Photonics 2 (2008) 185-189 Chinese patent: 发明专利( ZL200710099383.2 ) “ 降低 全光开关泵浦功率的方法、全光开关及其制备方法 ”
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Nature Photonics A strongly nonlinear photonic crystal with a wavelength-tunable bandgap could provide the solution to realizing all-optical switches for signal processing‘ ‘Controlling photons with light’
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IOP optics.org: ‘ Photonic crystals speed up all-optical switching’ A polystyrene photonic crystal that acts as an all- optical switch boasts picosecond response time and low power requirements. The picosecond switching time is impressive. 一种光子晶体开关以具备 皮秒时间响应和低泵浦功 率而值得自豪,皮秒的超 快开关时间令人印象深刻。
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Nature Asia Materials: Ultrafast Optical Switches: Now you see it, now you don’t Researchers from Peking University, China, now demonstrate fast all-optical switching in a photonic crystal made from a composite material.
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Nature China: “Optical Switches: A New Low” Qihuang Gong and co-workers at the Peking University in Beijing have devised a strategy for making ultrafast photonic- crystal-based optical switches that can operate under low- power pump light )。
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Response time: 35ps Switching efficiency: 65% Pump power: 230 KW/cm 2 Appl. Phys. Lett. 94, 031103 (2009) SPP resonant-enhancement 3) Nano-Ag:MEH-PPV PC optical switch
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PhysOrg.com: ‘ Nanocomposite material provides photonic switching’ The development of integrated photonic devices in tomorrow’s technology is taking place today at Peking University in Beijing, China, where a group of scientists has manufactured and tested nanocomposite material that could be used in integrated photonic devices
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Nanomaterials World : “Seeing the light” Nanomaterials world 5 (2009,Mar. 17) 5 Photonic devices could aid developments in computing, following research in China. The team from Peking University is working on a nanocomposite that could be integrated into photonic devices.
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IV. Conclusion ☆ An ultrafast low-power photonic crystal all-optical switch was realized by using the composite materials ☆ New composite materials are demonstrated to develop the 3rd optical nonlinearity ☆ Large 3 rd nonlinear susceptibility (4-orders enhanced ) and ultrafast response time ( of ps order ) were achieved
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Financial Supported by: NNSFC, China MOST, China MOE, China, Peking Uiversity V. Acknowledgement
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THE END Thank You!
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