Sensor based on Domain Inverted Electro-Optic

Similar documents
High Dynamic Range Electric Field Sensor for Electromagnetic Pulse Detection

High dynamic range electric field sensor for electromagnetic pulse detection

Bias-free Y-branch waveguide modulator based on domain-inversed modulation of electro-optic polymer

Demonstration of a Linearized Traveling Wave Y-Fed Directional Coupler Modulator Based on Electro-Optic Polymer

Optical Bus for Intra and Inter-chip Optical Interconnects

Polymer-based Hybrid Integrated Photonic Devices for Silicon On-chip Modulation and Board-level Optical Interconnects

LINEAR RING RESONATOR MODULATOR FOR MICROWAVE PHOTONIC LINKS

Guiding Light in Electro-Optic Polymers

Characterization of Photonic Structures with CST Microwave Studio. CST UGM 2010 Darmstadt

Frequency Dependent Harmonic Powers in a Modified Uni-Traveling Carrier (MUTC) Photodetector

Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane

Module 16 : Integrated Optics I

A Comparison of Optical Modulator Structures Using a Matrix Simulation Approach

Integrated Optical Waveguide Sensor for Lighting Impulse Electric Field Measurement

160MER, Austin, TX-78758, USA ABSTRACT 1. INTRODUCTION

Highly Linear, Broadband Optical Modulator Based on Electro-optic Polymer

Optoelectronic Oscillator Topologies based on Resonant Tunneling Diode Fiber Optic Links

Performance limitations of a Y-branch directionalcoupler-based. electro-optical modulator

Integration of Optoelectronic and RF Devices for Applications in Optical Interconnect and Wireless Communication

DIRECT MODULATION WITH SIDE-MODE INJECTION IN OPTICAL CATV TRANSPORT SYSTEMS

Electro-optic Electric Field Sensor Utilizing Ti:LiNbO 3 Symmetric Mach-Zehnder Interferometers

Integrated electro-optical waveguide based devices with liquid crystals on a silicon backplane

MANY research groups have demonstrated the use of silicon

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

RADIO-OVER-FIBER TRANSPORT SYSTEMS BASED ON DFB LD WITH MAIN AND 1 SIDE MODES INJECTION-LOCKED TECHNIQUE

Curriculum Vitae of Alan Xiaolong Wang

Linearized electrooptic directional coupler modulator in stoichiometric lithium niobate

Understanding RF and Microwave Analysis Basics

A continuously tunable and filterless optical millimeter-wave generation via frequency octupling

SHF Communication Technologies AG

High-Speed Optical Modulators and Photonic Sideband Management

EPIC: The Convergence of Electronics & Photonics

A NOVEL SCHEME FOR OPTICAL MILLIMETER WAVE GENERATION USING MZM

Photonic time-stretching of 102 GHz millimeter waves using 1.55 µm nonlinear optic polymer EO modulators

Finisar Contributors. Dave Adams Alan Chen Dingbo Chen Shiyun Lin Daniel Mahgerefteh Yasuhiro Matsui Thelinh Nguyen. 19 September

FREQUENCY MULTIPLIERS

High-speed Ge photodetector monolithically integrated with large cross silicon-on-insulator waveguide

Heterogeneously Integrated Microwave Signal Generators with Narrow- Linewidth Lasers

Antenna-coupled silicon-organic hybrid integrated photonic crystal modulator for broadband electromagnetic wave detection

Analog Characterization of Low-Voltage MQW Traveling-Wave Electroabsorption Modulators

772D coaxial dual-directional coupler 773D coaxial directional coupler. 775D coaxial dual-directional coupler 776D coaxial dual-directional coupler

Horizontal single and multiple slot waveguides: optical transmission at λ = 1550 nm

Mach Zehnder Interferometer True Time Delay Line

Testing with Femtosecond Pulses

Si CMOS Technical Working Group

Wavelength-controlled hologram-waveguide modules for continuous beam-scanning in a phased-array antenna system

S-band gain-clamped grating-based erbiumdoped fiber amplifier by forward optical feedback technique

Experimental analysis of two measurement techniques to characterize photodiode linearity

H.-W. Wu Department of Computer and Communication Kun Shan University No. 949, Dawan Road, Yongkang City, Tainan County 710, Taiwan

Near-Field Antenna Measurements using a Lithium Niobate Photonic Probe

Session 2: Silicon and Carbon Photonics (11:00 11:30, Huxley LT311)

A Broadband High-Efficiency Rectifier Based on Two-Level Impedance Match Network

Measuring Photonic, Optoelectronic and Electro optic S parameters using an advanced photonic module

A tunable Si CMOS photonic multiplexer/de-multiplexer

Silicon Photonics Technology Platform To Advance The Development Of Optical Interconnects

Large-Signal Modeling on Device Level: Intermodulation Distortion and Eye-Diagrams of Semiconductor Lasers

Progress In Electromagnetics Research Letters, Vol. 8, , 2009

Broadband Linearization Technologies for Broadband Radio-over-Fiber Transmission Systems

PHOTONIC INTEGRATED CIRCUITS FOR PHASED-ARRAY BEAMFORMING

InP-based Waveguide Photodetector with Integrated Photon Multiplication

Optical RI sensor based on an in-fiber Bragg grating. Fabry-Perot cavity embedded with a micro-channel

DESIGN OF LATTICE FORM OPTICAL DELAY LINE STRUCTURE FOR MICROWAVE BAND PASS FILTER APPLICATIONS

Traceability and Modulated-Signal Measurements

High Power RF MEMS Switch Technology

Mitigation of Nonlinear Spurious Products using Least Mean-Square (LMS)

Reconfigurable Front-End Modules Based on Ferroelectric Varactors

Bragg and fiber gratings. Mikko Saarinen

Development of LiNbO 3 for CATV Transmission Systems

Laser Transmitter Adaptive Feedforward Linearization System for Radio over Fiber Applications

Analysis of Stimulated Brillouin Scattering Characteristics in Frequency Domain

6 Electromagnetic Field Distribution Measurements using an Optically Scanning Probe System

Extending the Offset Frequency Range of the D2-135 Offset Phase Lock Servo by Indirect Locking

High-speed silicon-based microring modulators and electro-optical switches integrated with grating couplers

Examination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade:

Waveguide-based single-pixel up-conversion infrared spectrometer

HIGH-EFFICIENCY MQW ELECTROABSORPTION MODULATORS

ARTICLE IN PRESS. Optik 121 (2010) Simulative investigation of the impact of EDFA and SOA over BER of a single-tone RoF system

The Theta Laser A Low Noise Chirped Pulse Laser. Dimitrios Mandridis

Transmitting Light: Fiber-optic and Free-space Communications Holography

RF Over Fiber Design Guide Overview. Provided by OPTICAL ZONU CORPORATION

SPP waveguide sensors

Advanced Test Equipment Rentals ATEC (2832) Agilent 8510 System Solutions

STUDY OF LINEARIZATION OF OPTICAL POLYMER MODULATORS

Ultralinear heterogeneously integrated ring-assisted Mach Zehnder interferometer modulator on silicon

A GHz HIGH IMAGE REJECTION RATIO SUB- HARMONIC MIXER. National Cheng-Kung University, Tainan 701, Taiwan

Electro-Optic Sensors for RF Electric Fields: a Diagnostic Tool for Microwave Circuits and Antennas

New Focus High Speed Photoreceivers

Model Series 400X User s Manual. DC-100 MHz Electro-Optic Phase Modulators

2D silicon-based surface-normal vertical cavity photonic crystal waveguide array for high-density optical interconnects

Modulators. Digital Intensity Modulators. Analogue Intensity Modulators. 2.5Gb/sec...Page Gb/sec Small Form Factor...Page 3

arxiv: v1 [physics.optics] 19 Jun 2008

An Example Design using the Analog Photonics Component Library. 3/21/2017 Benjamin Moss

Optical IQ modulators for coherent 100G and beyond

LINEAR MICROWAVE FIBER OPTIC LINK SYSTEM DESIGN

A Frequency Reconfigurable Dual Pole Dual Band Bandpass Filter for X-Band Applications

CMOS 120 GHz Phase-Locked Loops Based on Two Different VCO Topologies

Hiroshi Murata and Yasuyuki Okamura. 1. Introduction. 2. Waveguide Fabrication

Broadband Beamforming of Terahertz Pulses with a Single-Chip 4 2 Array in Silicon

Broadband analog phase shifter based on multi-stage all-pass networks

Review on Various Issues and Design Topologies of Edge Coupled Coplanar Waveguide Filters

Transcription:

Large Dynamic Range Electromagnetic Field Sensor based on Domain Inverted Electro-Optic Polymer Directional Coupler Alan X. Wang Ray T. Chen Omega Optics Inc., Austin, TX -1-

Application of Electric Field Sensors: Electromagnetic Attack Alarming Medical Apparatuses Microwave-Integrated Circuit Testing Ballistic Control Health Protection (<100KHz) --

Electronic Sensor v.s. vs. Photonic Sensor Drawbacks of Conventional Electronic Sensor: Disturbance from electrical cables Narrow bandwidth Bulky size Advantages of Photonic EM Sensor: Free of disturbance to EM waves Broad bandwidth Compact size Precise measurement

Domain Inverted E-O Polymer Directional Coupler with Super High Dynamic Range DARPA MORPH E-O Polymer Domain Inverted Y-fed Directional Coupler -4-

What is E-O Polymer Materials? Chromophore + - Thin film - CLD1 V Host Polymer APC or PMMA Light ~ Pockels effect: Δn = 1 n 3 γe -5-

Materials Comparison Materials Polymers Si/SOI III-V LiNbO 3 Optical Loss (db/cm @1550nm) ~1 0. ~0.5 0. E-O efficiency (pm/v) 450 N/A <5 30 Bandwidth (GHz) 110 40 30 40 Fabrication Process Various CMOS RIE Ti diff. Integration Easy Standard Difficult No Cost Low Low Highest High Reliability Moderate High High High Improvement Potential Yes No No No -6-

Design of Domain Inverted E-O Polymer Directional Coupler Nonlinear Distortion in RF Photonics Signal RF Photonic link Signal + distortion E-O modulator Modulator f 1 f Third Order Intermodulation Distortion (IMD3) f 1 -f f -f 1 f 1 f RF I out = I0 I0 + cos[ φbias + Δφ( V )] Harmonic Signal -7-

Y-fed Directional Coupler based on Domain In erted Wa eguide Domain-Inverted Waveguide = = i i o R jb A jb A R M M R 1 1 1 R, S: Complex amplitude i i o S A jb A jb S S 1 1 1 H. Kogelnik and R. V. Schmidt, "Switches directional couplers with alternating ß", IEEE J. of Quantum Electron., vol. 1, pp. 396-401, July 1976 + = = = 1 1 ) ( n n h n V V f R Analytical Methods: Reduced simulation work Full spectrum coverage n n n dv V f d n h ) (! 1 = are the Taylor coefficients Full spectrum coverage Small errors -8-

Expression and amplitude of the signals from the Y-fed directional coupler Signal Frequency Amplitude (up to the 7th order expansion) DC 0 1/ Fundamental f 1, f 15 7 5 5 9 3 h7a + h5a + h3a + h1a 64 4 4 nd Harmonic f 1, f 0 IMD f 1 -f, f 1 +f 0 441 7 5 5 1 3rd Harmonic 3f 1, 3f h 7a + h5a + h3a 64 16 4 IMD3 f 1 -f, f -f 735 7 5 5 3 3 1 h 7a + h5a + h3a 64 8 4. 3 How to characterize the linearity of the optical modulators? V = a[sin( π f t) + sin(πf 1 t IMD3 is the most important t spurious signal because: It has the largest magnitude It is very close to the fundamental signals )] IMD3 suppression at 10% modulation depth

Design of Domain Inverted Modulator Schematic of the waveguide structure Simulation of the conversion length 3 μm.7 μm 3 μm UFC-170A LPD-80/APC, n=1.61, r 33 =80pm/V 0.5μm 5μm 10μm UV15-LV, n=1.49 Coupling length :lc=3.55mm at λ=1.55 μm -10-

Performances of YFDCs with different number of domains Name MZM Device 1 Device Device 3 Device 4 Type 1-domain 1-domain -domain 3-domain 4-domain Normalized Section Length s 1 =.8595 s 1 =.85 s =.85 85 s 1 =1.8859 s =1.5131 s 1 =.1884 s =.058 058 s 3 =.5464 s 3 =1.5383 s 4 =.6648 Average IMD3 43.6 51. 65. 97.5 110.3 suppression 10%~50% MD(dB) Driving Voltage 1.0.0.96 4.19 5.1 Maximum Modulation Depth 100% 7.6% 98% 96% 99.7% SFDR @ -145dB/Hz noise level(db/hz) 98 110 103 116 10 109 11 11 15 130 SFDR @-160dB/Hz noise level(db/hz) -11-

¾Device Fabrication UFC170A AJCJL1/APC V UV 15 LV UV 15 ~ ~ ~ ~ ~ ~ ~ Intrinsic silicon Hot plate -1-

Domain Inverted E-O Poling by Pulse Voltage Working Condition E-O poling direction EM Wave direction Top S S 1 +V Gold Gold Key Points: E-O poling without top cladding Domain inverted poling -V No bottom electrode Heavily Doped Silicon -13-

E-O Polymer Photonic EM Wave Sensor Characterization RF response @ 1GHz Xiaolong Wang, Beom-Suk Lee, Ray T. Chen, Large Dynamic Range Electromagnetic Field Sensor based on Domain Inverted Electro-Optic Polymer Directional Coupler, Invited Presentation, SPIE Photonics West conference, RF and Millimeter-Wave Photonics (Conference 7936), San Francisco, January -7, 7, 011

where ε 0 =8.854 10-1 F/m c=3 10 8 m/s E is the maximum amplitude of the electric field Minimum Electric Field 30V/m RF Power Density 0.3mW/cm Maximum 4 10 5 V/m 59KW/cm Solicitation Requirement: milliwatts per square centimeter to kilowatts per square centimeter Exactly Matched!

IMD3 Suppression MZ Modulator Fundamental IMD3 0dB 50dB Device 0: MZM Device 1: 1DM Y-fed DC Device : DM Y-fed DC Device 3: 3DM Y-fed DC Device 4: 4DM Y-fed DC Linear Modulator db higher h average IMD3 suppression from 10%~50% modulation depth 47dB higher IMD3 suppression @ 0% modulation depth Boem-Suk Lee, Che-Yun Lin, Xiaolong Wang, Jingdong Luo, Alex K.Y. Jen, and Ray T. Chen, Bias-free electro-optic polymer based two-section Y-branch waveguide modulator with -db linearity enhancement, Optics Letters, Vol.34, No.1, pp.377-379 (009) -16-

Spurious Free Dynamic Range MZ type Definition of Spurious Free Dynamic Range (SFDR) DC type Beomsuk Lee, Xiaolong Wang, Ray T. Chen, and Raluca Dinu, Electro-Optic Polymer Y-Brunch Directional Coupler Modulator with High Linearity, submitted to IEEE Photonic Technology Letters 11dB higher SFDR! -17-

Small Signal Modulation Measurement Laser Device EDFA 0 0 5 10 15 0 5 RF source λ=1.55μm Modulation depth = 4% Frequency range ~6.5GHz Photo detector onse (db) Respo -5-10 Microwave Spectrum -15 Analyzer -0 Frequency (GHz) 3-dB electrical bandwidth ~ 10GHz