Contains an introduction and reports on three research projects.Maryland Procurement Office Contract MDA 904-93-C4169Maryland Procurement Office Contract MDA 903-94-C6071U.S. Air Force - Office of Scientific Research Grant F49620-93-1-0604MIT Lincoln Laboratory Advanced Concepts Program Contract CX-16335U.S. Army Research Office Grant DAAH04-93-G-0399U.S. Army Research Office Grant DAAH04-93-G-018

Bounds, Jeffrey K.

Brothers, L. Reginald

Fung, Irene

Greer, Donald R.

Joneckis, Lance G.

Lai, Bobby Y.

Lee, Dicky

Mason, Elliott J.

Nee, Phillip T.

Patterson, Steven G.

Rediker, Robert H.

Shakeel, Asif

Shapiro, Jeffrey H.

Wong, Ngai C.

DSpace@MIT

Chapter 2. Optical Propagation and CommunicationChapter 2. Optical Propagation and CommunicationAcademic and Research StaffProfessor Jeffrey H. Shapiro, Dr. Robert H. Rediker, Dr. Ngai C. WongVisiting Scientists and Research AffiliatesDr. Lance G. Joneckis'Graduate StudentsJeffrey K. Bounds, L. Reginald Brothers, Irene Fung, Donald R. Greer, Bobby Y.Mason, Phillip T. Nee, Steven G. Patterson, Asif Shakeel2.1 Introduction 2.2.1 Quantum OpticalThe central theme of our programs has been toadvance the understanding of optical and quasi-optical communication, radar, and sensing systems.Broadly speaking, this has entailed: (1) developingsystem-analytic models for important optical propa-gation, detection, and communication scenarios; (2)using these models to derive the fundamental limitson system performance; and (3) identifying andestablishing through experimentation the feasibilityof techniques and devices which can be used toapproach these performance limits.2.2 Nonlinear and Quantum OpticsSponsorMaryland Procurement OfficeContract MDA 904-93-C4169Contract MDA 903-94-C6071Project StaffProfessor Jeffrey H. Shapiro, Dr. Ngai C. Wong, Dr.Lance G. Joneckis, Jeffrey K. Bounds, Elliott J.Mason, Phillip T. Nee, Steven G. Patterson, AsifShakeelLai, Dicky Lee, Elliott J.TapAn optical parametric amplifier (OPA) is a nearlyideal nonresonant generator of nonclassical light: itssignal and idler beams exhibit quantumentanglement which can be sensed as sub-shot-noise photon correlation or as a sub-shot-noisequadrature squeezing. It has been suggested thata gain-saturated OPA can provide a new route tononclassical light-beam generation,2  withoutrecourse to joint signal/idler measurements. In par-ticular, it may be possible to preserve the inputlarge-signal signal-to-noise ratio (SNR) of the ampli-fied channel in such an arrangement. Thus, aquantum optical tap for binary-phase-shift-keying(BPSK) could then be developed: such a tap wouldincur neither signal strength nor SNR degradation ineither of its output channels, i.e., its signal and tapoutput ports.As a prelude to demonstrating the precedingquantum optical tap concept, we have set up anultralow loss optical parametric oscillator (OPO) forstudy of quantum noise correlation. High qualitymirrors and a potassium titanyl phosphate (KTP)crystal have permitted stable cw operation of theOPO with a threshold of 30 mW. Another KTPOPO with a longer crystal and a two-piece lower-loss design has been found to have a threshold of20 mW. It is expected that the KTP OPOs shouldyield an intensity correlation between the signal andidler outputs of 90 percent and allow us to study themean-field characteristics, gain saturation, andquantum-noise spectra of an injection-seededOPA.31 Laboratory for Physical Sciences, College Park, Maryland.2 N.C. Wong, "Squeezed Amplification in a Nondegenerate Parametric Amplifier," Opt. Lett. 16(21): 1698-1700 (1991).3 K.-X. Sun, Classical and Quantized Fields in Optical Parametric Interactions, Ph.D. diss., Dept. of Physics, MIT, 1993.143Chapter 2. Optical Propagation and CommunicationWe have begun an experiment to resonantly gen-erate the second harmonic of a 500-mW 1.06 pmYAG laser. The goal is to obtain stable cw opera-tion and a high conversion efficiency of 60-80percent in the second-harmonic generation. If suc-cessful, this arrangement will serve as a compact,low-noise pump source for KTP OPOs. Moreover,for degenerate OPO operation, the YAG laser canbe used as the local oscillator for homodynedetection of quadrature-noise squeezing.2.2.2 Quasi-Phase Matched NonlinearOpticsWe have initiated a study of quasi-phase matching(QPM) 4 in lithium niobate with the goal of fabricatingQPM nonlinear optical devices that can be operatedat any user specified wavelength, such as in the 1.5pm optical communication window. Nonlinearoptical devices that are fabricated using QPM arepotentially useful in many applications, such asoptical frequency conversion and amplification foroptical communication networks. By employing theelectric field poling technique,5 we have success-fully obtained domain reversal in a bulk250-pm-thick lithium niobate sample. To achieveQPM it is necessary to obtain a periodic gratingpattern of regular and domain reversed material inlithium niobate with a grating period of 5-15 pmmaintained over a length of 1 cm. We are in theprocess of fabricating domain-reversed material in aperiodic grating pattern.2.2.3 Squeezed-State Generation in OpticalFiberIn theoretical work, we have been establishing thelimits on squeezed-state generation in optical fiber.Recently, we have shown that the Raman noisewhich accompanies the noninstantaneous Kerreffect sets a new limit on the degree of quadrature-noise squeezing that can be obtained fromcontinuous-wave four-wave mixing in optical fiber.6For pulsed squeezed-state generation in fiber, wehave shown that local-oscillator (LO) pulse com-pression is the key to observing the full squeezinggenerated when the nonlinear interaction is pumpedby a transform-limited Gaussian pulse.7 We are nowworking on the theory of optimal LO selection forquadrature-noise measurements of arbitrary spatio-temporal quantum states.2.2.4 Quantum Phase MeasurementsRecently, a great deal of attention has been givento the phase problem for a single-mode quantumfield. Previously, we showed that there are signif-icant physical differences-with potentially importantpractical consequences-that emerge if the focus inphase-based quantum communication and precisionmeasurement is shifted from single-mode fields totwo-mode fields.8 In particular, with a two-modefield it is possible to achieve perfect (i.e., zero errorprobability) K-ary phase-based digital communica-tion at a root-mean-square (rms) photon number ofK/2. This same rms photon number is also suffi-cient for a phase-based precision measurement ofa c-number phase shift whose observation error isguaranteed to be no more than - Tr/K. The capa-bilities of these schemes for phase-based digitalcommunication and precision measurement are rad-ically different from those of their single-modecounterparts. Indeed, in single-mode phase-basedcommunication it is impossible to achieve zeroerror probability at finite average photon number.Likewise, a single-mode phase measurement atfinite average photon number cannot realizeprobability-one confinement of the measurementerror to any proper subinterval of (- Tr, rr].The two-mode phase measurement scheme refer-enced above relies on generating an entangledstate, and the use of a quantum measurementwhich is the two-mode generalization of theSusskind-Glogower probability operator measure.As yet, there are no explicit approaches availablefor realizing either of these abstractions. In our4 M.M. Fejer, G.A. Magel, D.H. Jundt, and R.L. Byer, "Quasi-Phase-Matched Second Harmonic Generation: Tuning and Tolerances,"IEEE J. Quantum Electron. 28(11): 2631-2654 (1992).5 M. Yamada, N. Nada, M. Saitoh, and K. Watanabe, "First-Order Quasi-Phase Matched LiNbO3 Waveguide Periodically Poled byApplying an External Field for Efficient Blue Second-Harmonic Generation," Appl. Phys. Lett. 62(5): 435-436 (1993).6 J.H. Shapiro and L. Boivin, "Raman-Noise Limit on Squeezing Continuous Wave Four-Wave Mixing," Opt. Lett., forthcoming.7 L.G. Joneckis and J.H. Shapiro, "Enhanced Fiber Squeezing via Local-Oscillator Pulse Compression," Proceedings of NonlinearOptics: Materials, Fundamentals and Applications, Waikaloa, Hawaii, July 24-29, 1994.8 J.H. Shapiro, "Phase Conjugate Quantum Communication with Zero-Error Probability at Finite Average Photon Number," Phys.Script. T48: 105-112 (1993).144 RLE Progress Report Number 137present program, however, we have relieved themeasurement part of this realization burden. Spe-cifically, we have shown that zero error probabilityphase-based digital communication and ± Tr/Kaccuracy phase-based precision measurement canbe accomplished-at an average photon number ofapproximately K3/2 -via optical heterodynedetection.9 Again, an appropriate two-mode entan-gled state is needed for which a generation tech-nique is currently being sought.2.2.5 PublicationsJoneckis, L.G., and J.H. Shapiro. "Enhanced FiberSqueezing via Local-Oscillator Pulse Com-pression." Proceedings of Nonlinear Optics:Materials, Fundamentals and Applications.Waikaloa, Hawaii, July 24-29, 1994.Shapiro, J.H. "An Eclectic Tour of Quantum OpticalCommunications." Invited paper presented atthe 1994 Annual Meeting of the Optical Societyof America, Dallas, Texas, October 2-7, 1994.Shapiro, J.H. "Phase Conjugate Quantum Commu-nication with Optical Heterodyne Detection."Opt. Lett. Forthcoming.Shapiro, J.H., and L. Boivin. "Raman-Noise Limit onSqueezing continuous Wave Four-WaveMixing." Opt. Lett. Forthcoming.Shapiro, J.H., and K.-X. Sun. "Semiclassical versusQuantum Behavior in Fourth-Order Interfer-ence." Proceedings of Nonlinear Optics: Mate-rials, Fundamentals and Applications, Waikaloa,Hawaii, July 24-29, 1994.Shapiro, J.H., and K.-X.Quantum Behaviorence." J. Opt. Soc.(1994).Sun. "Semiclassical versusin Fourth-Order Interfer-Am. B 11(6): 1130-1141Chapter 2. Optical Propagation and Communication2.3 Multiresolution Laser Radar RangeProfilingSponsorU.S. Air Force - Office of Scientific ResearchGrant F49620-93-1-0604Project StaffProfessor Jeffrey H. Shapiro, Irene Fung, Donald R.GreerThis effort is part of a collaboration on automatictarget detection and recognition, with ProfessorsAlan S. Willsky (from MIT's Laboratory for Informa-tion and Decision Systems) and W. Eric L. Grimson(from MIT's Artificial Intelligence Laboratory) andtheir students. The unifying theme of the collab-oration is the use of multiresolution (wavelet)methods at every stage-from sensor front-endprocessing, through feature extraction, to the objectrecognition module-in an overall system. Our ownactivity centers on the application of multiresolutiontechniques to laser radars. Previously, we havestudied maximum-likelihood (ML) estimation forplanar range-profiling with a laser radar. 10 Theimportance of the ML approach lies in its ability tosuppress the range anomalies caused by laserspeckle. The practicality of the ML approachderives from the utility of the expectation-maximization (EM) algorithm for this problem. Inthe current program, we have shown that the sameEM approach can be applied, at any desiredwavelet scale, to perform ML profiling. Using theHaar wavelet basis, we have demonstrated the useof this technique on simulated laser-radar rangedata."1 In this study, we have established an effi-cient, weight-based stopping rule for terminating thecoarse-to-fine progression of multiresolution MLestimation. We are presently working on improvingthe computational efficiency of our ML/EM approachso that this technique can be applied to real laser-radar test bed data from the Opto-Radar SystemsGroup of MIT Lincoln Laboratory.9 J.H. Shapiro, "Phase Conjugate Quantum Communication with Optical Heterodyne Detection." Opt. Lett., forthcoming.10 T.J. Green, Jr., and J.H. Shapiro, "Maximum-Likelihood Laser Radar Range Profiling with the Expectation-Maximization Algorithm,"Opt. Eng. 31(11) 2343-2354 (1992)11 I. Fung and J.H. Shapiro, "Multiresolution Laser Radar Range Profiling with the Expectation-Maximization Algorithm," Proceedings ofthe Joint A TR Systems and Technology Conference IV, Monterey, California, November 14-18, 1994.145Chapter 2. Optical Propagation and Communication2.3.1 PublicationsFung, I.withS.M.Sci.,Multiresolution Laser Radar Range Profilingthe Expectation-Maximization Algorithm.thesis. Dept. of Electr. Eng. and Comput.MIT, 1994.Fung, I., and J.H. Shapiro. "Multiresolution LaserRadar Range Profiling with the Expectation-Maximization Algorithm." Proceedings of theJoint A TR Systems and Technology ConferenceIV, Monterey, California, November 14-18, 1994.2.4 Optical Frequency Division andSynthesisSponsorsMIT Lincoln LaboratoryAdvanced Concepts ProgramContract CX-16335U.S. Army Research OfficeGrant DAAH04-93-G-0399Grant DAAH04-93-G-0187Project StaffDr. Ngai C. Wong, L. Reginald Brothers, Bobby Y.Lai, Dicky LeeFrequency division and synthesis in the opticaldomain play an important role in modern opticalprecision measurements, optical frequency stand-ards, and coherent optical communication. Thefocus of this program is to study the feasibility ofestablishing an optical frequency counter based ona parallel network of phase-locked opticalparametric oscillators (OPOs). It includes thedevelopment of a number of enabling technologies,such as wideband optical frequency comb (OFC)generation, 12 tunable cw OPOs, 13 and techniquesfor operating a parallel network of OPOs. AnOPO-based optical frequency counter can be oper-ated to measure, compare, and synthesize frequen-cies from optical to microwave, with high precisionand accuracy.2.4.1 Terahertz Optical Frequency CombGenerationIn order to facilitate difference-frequency measure-ments in the terahertz range, we have developedan optical frequency comb (OFC) generator basedon an efficient electro-optic phase modulatordesign. By incorporating a microwave waveguideresonator structure in a LiNbO3 electro-opticmodulator, the phase velocities of the microwaveand optical fields can be matched to maximize theelectro-optic modulation at a user-specified micro-wave frequency. The modulation is furtherenhanced by placing the modulator inside an opticalcavity that is resonant for the input optical beamand the generated sidebands. For 1 W of micro-wave power at 17 GHz, we have obtained anoptical frequency comb with a 3-THz span. 12We have investigated the effects of small micro-wave frequency detuning on the OFC spectrum.Without detuning a symmetric spectrum is obtainedand the span of 3 THz is entirely limited by the dis-persion of the lithium niobate crystal. By detuning+2.3 MHz, we have observed an asymmetric spec-trum, expanding towards the shorter wavelengthsand contracting from the longer wavelengthsbecause the detuning brings the shorter wave-lengths into resonance and the longer wavelengthsout of resonance. The one-sided span toward theshorter wavelengths is found to be 2.3 THz. Furtherdetuning returns the spectrum to a symmetricshape but with a much smaller span. By using posi-tive and negative detuning it is therefore possible toextend the OFC spectrum to a span of 4.6 THz. Weare presently working on compensating the disper-sion in order to extend the spectrum span to 10THz or more.2.4.2 Tunable Optical Parametric OscillatorOptical parametric generation has been well knownfor producing tunable radiation over a broad spec-tral range. This has been realized in pulsed OPOsbut not in cw OPOs. The doubly-resonant conditionin cw operation, in which both the signal and idlerwaves are resonant with the cavity, prevents contin-uous frequency tuning. A singly resonant cw OPOcan be tuned continuously, but at the expense of amuch higher threshold power. We have developeda novel dual-cavity configuration that retains the12 L.R. Brothers, D. Lee, and N.C. Wong, "Terahertz Optical Frequency Comb Generation and Phase Locking of Optical ParametricOscillator at 665 GHz," Opt. Lett. 19(4): 245-247 (1994).13 D. Lee and N.C. Wong, "Tunable Optical Frequency Division using a Phase-Locked Optical Parametric Oscillator," Opt. Lett. 17(1):13-15 (1992).146 RLE Progress Report Number 137low-threshold capability of an ordinary doubly-resonant system, and at the same time is capableof continuous tuning. By employing two separatecavities to resonate the signal and idler waves inde-pendently, the output frequencies become contin-uously tunable. Experimentally, we have observeda tuning range of 1 GHz, which is 100 times morethan a single-cavity OPO. Theoretically, the tuningrange is limited only by the phase-matching band-width of the nonlinear crystal, which is about 50-100GHz for KTP.We have discovered that the limiting factors for thetuning range are the weak pump resonance and theresonant leakage between the two cavities. As theOPO is tuned, the weak resonance of the pumpfield reduces the circulating pump intensity to alevel below the threshold, thus effectively limitingthe tuning range. Leakage of the signal and idlerwaves is caused by the imperfect coating of thepolarizing beam splitter that is used to separate thesignal and idler beams. Resonant leakage occurswhen the idler cavity is resonant with the leakedsignal field, which effectively leads to a lossy signalcavity, and vice versa. Lossy cavities increase thethreshold and hence limit the tuning range. We arein the process of minimizing their effects by utilizingthe angle walkoff of KTP to separate the twobeams, thus eliminating the polarizing beam andimproving the tuning range.2.4.3 Three-Wave Mixing in CTAIt is potentially useful to have a tunable source at1.5 pm for optical communications. We have useda new nonlinear optical crystal, cesium titanylarsenate (CTA), to generate tunable radiation bythree-wave difference-frequency mixing. 14 By usinga krypton ion laser at 531 nm as the pump and atunable Ti:sapphire laser as the input signal, wehave generated 1 pW of tunable radiation from1567 nm to 1653 nm. The use of a resonant cavityfor frequency mixing has yielded an output power ofChapter 2. Optical Propagation and Communication-100 pW. We have also determined that the CTAphase-matching angle for generating a 3-to-1 OPOfrequency divider pumped at 532 nm is8 = 900, 0 = 480. We have not observed parametricoscillation due to the quality of the crystal. We arepresently investigating the use of other nonlinearcrystals with better crystal quality such as lithiumborate for demonstrating a 3-to-1 OPO.2.4.4 PublicationsBrothers, L.R., D. Lee, and N.C. Wong. "TerahertzOptical Frequency Comb Generation and PhaseLocking of Optical Parametric Oscillator at 665GHz." Opt. Lett. 19(4): 245-247 (1994).Lee, D., and N.C. Wong. "Tuning Characteristics ofa cw Dual-Cavity KTP Optical ParametricOscillator." Paper presented at the Conferenceon Lasers and Electro-Optics, Anaheim,California, May 8-13, 1994.Wong, N.C., and D. Lee. "Frequency Tuning andPhase Locking of an Ultrastable Doubly Reso-nant Optical Parametric Oscillator." Paper pre-sented at the Advanced Solid-State lasersTopical Meeting, Salt Lake City, Utah, February7-10, 1994.Wong, N.C., D. Lee, and L.R. Brothers. "Cw Phase-Locked Optical Parametric Oscillator as aTunable Source for Terahertz Radiation." Pro-ceedings of the SPIE Nonlinear Optics for High-Speed Electronics, Los Angeles, California,January 25, 1994.Wong, N.C., D. Lee, L.R. Brothers, and B. Lai."Optical Frequency Measurement and Synthesisusing Nonlinear Optical Techniques." Invitedpaper presented at the Conference on Lasersand Electro-Optics, Anaheim, California, May8-13, 1994.14 B.Y.F. Lai, A Tunable Light Source at 1.6 pm by Difference-Frequency Mixing in Cesium Titanyl Arsenate, S.M. thesis, Dept. ofElectr. Eng. and Comput. Sci., MIT, 1995.Professor Qing Hu (Photo by John F. Cook)148 RLE Progress Report Number 137

Optical Propagation and Communication

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