Definition of the Subject
Since its conception in 1958, the laser has become a nearlyubiquitous feature of the technological landscape finding its wayinto a spectacular array of devices from data storage toentertainment to fundamental science and metrology and myriadothers. One of the principal features of the laser is itsremarkable coherence. It is a nearly ideal source of monochromaticradiation and from this property the fields of precisionspectroscopy and timekeeping have reaped huge rewards. Recently, aninnovation in the design of a class of ultrashort-pulse lasers hasresulted in a new type of optical clockwork with stability thatrivals and even supercedes that of the best atomic clocks, includingthe cesium-beam clocks which, by international agreement, are usedto define the second. The nearly perfect train of optical pulsesemitted from these laser clocks are associated with a nearly idealspectrum of periodic spikes, or comb-lines, in the opticalfrequency...
Abbreviations
- First and second laser thresholds:
-
Minimum conditions forproducing stable and chaotic laser operation, respectively.
- Lorenz equations:
-
A system of three coupled nonlineardifferential equations describing convective fluid flow incells. These equations and their solutions launched the field of chaostheory.
- Modelocked laser:
-
A laser with evenly spaced modes which havetheir phases locked together so that the superposition of the modescreates a periodic train of very short pulses \( { <1\,\mathrm{ps} } \)).
- Poisson photon distribution:
-
Probability of k photons arrivingin a given interval of time for which there are an average of \( { \bar n } \)photons.
- Relaxation oscillation:
-
Periodic fluctuation about anequilibrium point when a system, initially operating in steady-state,is subjected to a transient perturbation. The system “relaxes” backto equilibrium through a (usually) damped sinusoidal response.
- Shot noise:
-
Noise produced by the random arrival of electrons ina photodetector illuminated by a laser field.
- Soliton:
-
A solitary wave packet which is a solution toa nonlinear wave equation in a medium possessing both dispersion andnonlinearity. These effects balance exactly so that the wave packetmaintains its shape and is stable against perturbations.
Bibliography
Barnes JA, Chi AR, Cutler LS, Healey DJ, LeesonDB, McGunigal TE, Mullen JA Jr, Smith WL, Sydnor RL, Vessot RFC,Winkler GMR (1971) Characterization of frequency stability. IEEETrans Instrum Meas IM-20:105–120
Kroupa VF (ed) (1983) Frequency stability:Fundamentals and measurement. IEEE Press, New York
Sullivan DB, Allan DW, Howe DA, Walls FL (eds)(1990) Characterization of clocks and oscillators: NIST Technical Note1337. United States Government Printing Office, Washington
Siegman AE (1986) Lasers. University ScienceBooks, Mill Valley
Milonni PW, Shih M, Ackerhalt JR (1987) Chaos inLaser-Matter Interactions. World Scientific, Singapore
Narducci LM, Abraham NB (1988) Laser Physics andLaser Instabilities. World Scientific, Singapore
Saleh BEA, Teich MC (1991) Fundamentals ofPhotonics. Wiley, New York
Svanberg S (1992) Atomic and MolecularSpectroscopy, 2nd edn. Springer, Berlin
Demtröder W (1996) Laser Spetroscopy, 2ndedn. Springer, Berlin
Yariv A (1997) Optical Electronics in ModernCommunications, 5th edn. Oxford University Press, Oxford
Koechner W (1996) Solid State Laser Engineering,4th edn. Springer, Berlin
Haken H (1985) Light. In: Laser Dynamics, vol 2. North-Holland, Amsterdam
Boyd RW, Raymer MG, Narducci LM (eds) (1986) OpticalInstabilities. In: Proceedings of the International Meeting onInstabilities and Dynamics of Lasers and Nonlinear Optical Systems,University of Rochester, 18–21 June, 1985. Cambridge UniversityPress, Cambridge
Abraham NB, Mandel P, Narducci LM (1988)Dynamical instabilities and pulsations in lasers. In: Wolf E (ed)Progress in Optics, vol XXV, ch. I. North-Holland, Amsterdam,pp 1–190
Robins WP (1982) Phase Noise in Signal Sources.Peter Peregrinus, London
Weiss CO, Vilaseca R (1991) Dynamics ofLasers. Weinheim, New York
Riehle F (2004) Frequency Standards. Wiley-VCH,Weinheim
Kärtner FX, Morgner U, Schibli T, Ell R, Haus HA,Fujimoto JG, Ippen EP (2004) Few-Cycle Pulses Directly froma Laser. In: Topics in Applied Physics, vol 95. Springer, Berlin,pp 73–136
Ye J, Cundiff ST (eds) (2005) Femtosecond OpticalFrequency Comb Technology: Principle, Operation and Application.Springer, New York
Jackson JD (1999) Classical Electrodynamics, 3rdedn. Wiley, New York
Slichter CP (1963) Principles of MagneticResonance. Harper and Row, New York
HechtE (2002) Optics, 4th edn. Addison-Wesley, SanFrancisco
van Tartwijk GHM, Agrawal GP (1998) Laserinstabilities: a modern perspective. Prog Quant Elect 22:43–122
Dunsmuir R (1961) Theory of relaxationoscillations in optical masers. J Electron Contr 10:453–458
Begon M, Harper JL, Townsend CR (1986) Ecology:Individuals, Populations, and Communities. Sinauer Assoc, Sunderland
Davis HT (1962) Introduction to NonlinearDifferential and Integral Equations. Dover, New York
Kaplan JI, Zier R (1962) Model for transientoscillations in a three-level optical maser. J Appl Phys 33:2372–2375
Bostick HA, O'Connor JR (1962) Infrared oscillationsfrom CaF2:U+3 and BaF2:U+3 masers. Proc IRE50:219–220
Tang CL (1963) On maser rate equations and transientoscillations. J Appl Phys 34:2935–2940
Lorenz EN (1963) Deterministic nonperiodic flow. J Atmos Sci 20:130–141
Gleick J (1987) Chaos. Penguin, New York
Schuster HG, Just W (2005) Deterministic Chaos,4th edn. Wiley-VCH, Weinheim
Haken H (1975) Analogy between higher instabilitiesin fluids and lasers. Phys Lett 53A:77–78
Casperson LW (1978) Spontaneous coherentpulsations in laser oscillators. IEEE J Quantum ElectronQE-14:756–761
Mayr M, Risken H, Vollmer HD (1981) Periodic and chaoticbreathing of pulses in a ringlaser. Optics Comm 36:480–482
Weiss CO, Klische W (1984) On observability of Lorenzinstabilities in lasers. Optics Comm 51:47–48
Lugiato LA, Narducci LM, Bandy DK, Pennise CA(1983) Breathing, spiking and chaos in a laser with injected signal.Opt Commun 46:64–68
Weiss CO, Godone A, Olafsson A (1983) Routes tochaotic emission in a cw He-Ne laser. Phys Rev A 28:892–895
Arrechi FT, Lippi GL, Puccioni GP, Tredicce JR (1984)Deterministic chaos in laser with injected signal. Optics Comm51:308–314
Shih M, Milonni PW, Ackerhalt JR (1985) Modelinglaser instabilities and chaos. J Opt Soc Amer B 2:130–135
Narducci LM, Sadiky H, Lugiato LA, Abraham NB (1985)Experimentally accessible periodic pulsations of a single-modehomogeneously broadened laser (the Lorenz model). Optics Comm 55:370
Weiss CO, Brock J (1986) Evidence for Lorenz-type chaosin a laser. Phys Rev Lett 57:2804–2806
Pujol J, Laguarta F, Vilaseca R, Corbalán R (1988)Influence of pump coherence on the dynamic behavior of a laser. J OptSoc Amer B 5:1004–1010
Lauterborn W, Steinhoff R (1988) Bifurcation structureof a laser with pump modulation. J Opt Soc Amer B 5:1097–1104
Brunner W, Fischer R, Paul H (1988) Time evolution ofthe total electric-field strength in multimode lasers. J Opt Soc AmerB 5:1139–1143
Khanin YI (1988) Mechanisms of nonstationary behavior ofsolid-state lasers. J Opt Soc Amer B 5:889–898
Abraham NB, Allen UA, Peterson E, Vicens A, Vilaseca R,Espinosa V, Lippi GL (1995) Structural similarities and differencesamong attractors and their intensity maps in the Laser-Lorenzmodel. Optics Comm 117:367–384
Smith CP, Dykstra R (1996) Observation in the two-levelspatial Maxwell-Bloch model of the anomalously large first peak asseen in experimental Lorenz-like spiral chaos from the 15NH3laser. Optics Comm 129:69–74
Lauterborn W, Kurz T (2003) Coherent Optics, 2ndedn. Springer, Berlin
Mørk J, Mark J, Tromborg B (1990) Route to chaos andcompetition between relaxation oscillations for a semiconductor laserwith optical feedback. Phys Rev Lett 65:1999–2002
Hentschel M, Kienberger R, Spielmann C, ReiderGA, Milosevic N, Brabec T, Corkum P, Heinzmann U, Drescher M, Krausz F(2001) Attosecond metrology. Nature 414:509–513
Diels J-C, Rudolf W (1996) Ultrashort Laser PulsePhenomena. Academic Press, San Diego
Scott A (2003) Nonlinear Science; Emergence andDynamics of Coherent Structures, 2nd edn. Oxford University Press,Oxford
Korteweg DJ, deVries G (1895) On the change of form oflong waves advancing in a rectangular canal, and on a new type of longstationary waves. Philos Mag Ser 5 39:422–443
Russell JS (1838) Report of the committee onwaves. Report of the 7th Meeting of the British Association for theAdvancement of Science, pp 417–496
Lamb GL Jr (1980) Elements of Soliton Theory. Wiley, New York
Ablowitz MJ, Segur H (1981) Solitons and the InverseScattering Transform. Society for Industrial and Applied Mathematics,Philadelphia
Zabusky NJ, Kruskal MD (1965) Interaction of“solitons in a collisionless plasma and the recurrence of initialstates”. Phys Rev Lett 15:240–243
Scott AC, Chu FYF, McLaughlin DW (1973) Thesoliton – a new concept applied science. Proc IEEE 61:1443–1483
Hasegawa A, Tappert F (1973) Transmission of stationarynonlinear optical pulses in dispersive dielectric fibers. I. Anonalousdispersion. Appl Phys Lett 23:142–144
Mollenauer LF, Stolen RH, Gordon JP (1980) Experimentalobservation of picosecond pulse narrowing and solitons in opticalfibers. Phys Rev Lett 45:1095–1098
Haus HA (1975) Theory of mode locking with a fastsaturable absorber. J Appl Phys 46:3049–3058
Haus HA, Fujimoto JG, Ippen EP (1991) Structures foradditive pulse modelocking. J Opt Soc Amer B 8:2068–2076
Haus HA, Fujimoto JG, Ippen EP (1992) Analytic theory ofadditive pulse and Kerr lens mode locking. IEEE J Quantum Electron28:2086–2096
Haus HA, Mecozzi A (1993) Noise of mode-lockedlasers. IEEE J Quantum Electron 29:983–996
Kapitula T, Kutz JN, Sandstede B (2002) Stability ofpulses in the master mode-locking equation. J Opt Soc Amer B19:740–746
Menyuk CR, Wahlstrand JK, Willits J, Smith RP, SchibliTR, Cundiff ST (2007) Pulse dynamics in mode-locked lasers:relaxation oscillations and frequency pulling. Opt Express15:6677–6689
Papoulis A (1965) Probability, Random Variables,and Stochastic Processes. McGraw-Hill, New York
Cooper GR, McGillem CD (1971) ProbabilisticMethods of Signal and System Analysis, 2nd edn. Holt, Rinehart andWinston, Fort Worth
Schawlow AL, Townes CH (1958) Infraredand optical masers. Phys Rev 112:1940–1949
Salomon C, Hils D, Hall JL (1988) Laserstabilization at the millihertz level. J Opt Soc Amer B 5:1576–1587
Eichenseer M, von Zanthier J, Walther H (2005)Common-mode-free frequency comparison of lasers with relativefrequency stability at the millihertz level. Opt Lett 30:1662–1664
Notcutt M, Ma L-S, Hall JL (2005) Simple and compact 1?Hzlaser system via an improved mounting configuration of a referencecavity. Opt Lett 30:1815–1817
Loudon R (1973) The Quantum Theory of Light. OxfordUniversity Press, Oxford
Kingston RH (1995) Optical Sources, Detectors,and Systems. Academic Press, San Diego
Feller W (1957) An Introduction to Probability Theoryand Its Applications. Wiley, New York, p 168
Gradshteyn IS, Ryzhik IM (1980) Table of Integrals,Series, and Products, corrected and enlarged 4th edn. Academic Press, New York
Abramowitz M, Stegun IA (eds) (1965)Handbook of Mathematical Functions, 55. US Department of Commerce,National Bureau of Standards, Washington
Scott RP, Langrock C, Kolner BH (2001) Highdynamic range laser amplitude and phase noise measurement techniques.IEEE J Select Topics Quant Electron 7:641–655
Kluge J, Wiechert D, Linde DV (1984) Fluctuationsin synchronously modelocked dye lasers. Opt Commun 51:271–277
Helbing FW, Steinmeyer G, Keller U, Windeler RS, StengerJ, Telle HR (2002) Carrier-envelope offset dynamics of modelockedlasers. Opt Lett 27:194–196
Scott RP, Kolner BH, Langrock C, Byer RL, Fejer MM(2003) Ti: sapphire laser pump-noise transfer function. In:Proceedings of the Conference on Lasers and Electro-optics, PaperCFB2, Baltimore
Kolner BH, Scott RP, Langrock C (2003) Laser phasenoise degradation from thermal effects due to pump powerfluctuations. In: Proceedings of the 2003 IEEE/LEOS Summer TopicalMeeting on Photonic Time/Frequency Measurement and Control, PaperTuC3.3, Vancouver, Institute of Electrical andElectronics Engineers, 14–16 July
Mulder TD, Scott RP, Baker KA, Kolner BH (2007)Characterization of the complex noise transfer function ofa modelocked Ti:sapphire laser. In: Conference on Lasers andElectro-Optics (CLEO 2007), Baltimore, Paper JThD38
Scott RP, Mulder TD, Baker KA, Kolner BH (2007)Amplitude and phase noise sensitivity of modelocked Ti:sapphire lasersin terms of a complex noise transfer function. Opt Express15:9090–9095
Weber R, Neuenschwander B, Donald MM, Roos MB,Weber HP (1998) Cooling schemes for longitudinally diode laser-pumpedNd:YAG rods. IEEE J Quantum Electron 34:1046–1053
Kolner BH (2008) Dynamic temperature distribution incylindrical laser rods with time-varying pump sources. (inpreparation)
Kolner BH, Mulder TD, Scott RP (2008) Laser noisemodulation transfer functions. (in preparation)
Mulder TD, Scott RP, Kolner BH (2008)Amplitude and envelope phase noise of a modelocked laser predictedfrom its noise transfer function and the pump noise power spectrum.Opt Express 16(18):14186–14191
Bender CM, Orszag SA (1978) Advanced MathematicalMethods for Scientists and Engineers. McGraw-Hill, New York
Haus HA, Lai Y (1990) Quantum theory of solitonsqueezing: a linearized approach. J Opt Soc Amer B 7:386–392
Haberman R (1987) Elementary Applied PartialDifferential Equations with Fourier Series and Boundary ValueProblems, 2nd edn. Prentice-Hall, New Jersey
Kuizenga DJ, Siegman AE (1970) FM and AM mode locking ofthe homogeneous laser – Part I: Theory. IEEE J Quantum ElectronQE-6:694–708
Kuizenga DJ, Siegman AE (1970) FM and AM mode locking ofthe homogeneous laser – Part II: Experimental results in a Nd:YAG laserwith internal FM modulation. IEEE J Quantum Electron QE-6:709–715
Scavennec A (1976) Mismatch effects in synchronouspumping of the continuously operated mode-locked laser. Optics Comm17:14–17
Zheng JP, Sen U, Benenson DM, Kwok HS (1986) Observationof periodicity multiplication in a synchronously pumped dye laser.Opt Lett 11:632–634
MacFarlane DL, Casperson LW (1987) Pulse-traininstabilities in a mode-locked argon laser: Experimental studies. J Opt Soc Amer B 4:1777–1780
MacFarlane DL, Casperson LW, Tovar AA (1988) Spectralbehavior and pulse train instabilities of a synchronously pumpedmode-locked dye laser. J Opt Soc Amer B 5:1144–1152
Scott RP, Bennett CV, Kolner BH (1997) AM andhigh-harmonic FM modelocking. Appl Opt 36:5908–5912
Valdmanis JA, Fork RL, Gordon JP (1985) Generation ofoptical pulses as short as 27 femtoseconds directly from a laserbalancing self-phase modulation, group-velocity dispersion, saturableabsorption, and saturable gain. Opt Lett 10:131–133
Avramopoulos H, French PMW, Williams JAR, New GHC,Taylor JR (1988) Experimental and theoretical studies of complex pulseevolutions in a passively mode-locked ring dye laser. IEEE J QuantumElectron 24:1884–1892
Spence DE, Kean PN, Sibbett W (1991) 60-fsec pulsegeneration from a self-modelocked Ti-sapphirelaser. Opt Lett16:42–44
Christov IP, Kapteyn HC, Murnane MM, Huang C-P, Zhou J(1995) Space-time focusing of femtosecond pulses in a Ti:sapphirelaser. Opt Lett 20:309–311
Kalosha VP, Müller M, Herrmann J, Gatz S (1998)Spatiotemporal model of femtosecond pulse generation in Kerr-lensmode-locked solid-state lasers. J Opt Soc Amer B 15:535–550
Christov IP, Stoev VD (1998) Kerr-lens mode-lockedlaser model: role of space time effects. J Opt Soc Amer B15:1960–1966
Jirauschek C, Kärtner FX, Morgner U (2003)Spatiotemporal Gaussian pulse dynamics in Kerr-lens mode-lockedlasers. J Opt Soc Amer B 20:1356–1368
Sergeev AM, Vanin EV, Wise FW (1997) Stability ofpassively modelocked lasers with fast saturable absorbers. Optics Comm140:61–64
Liu Y-M, Prucnal PR (1993) Slow amplitude modulation inthe pulse train of a self-modelocked Ti:sapphire laser. IEEE JQuantum Electron 29:2663–2669
Sucha G, Bolton SR, Weiss S, Chemla DS (1995) Perioddoubling and quasi-periodicity in additive-pulse mode-lockedlasers. Opt Lett 20:1794–1796
Sánchez LM, Hnilo AA (2001) Description of Kerr lensmode-locked lasers with Poincaré maps in the complex plane. OpticsComm 199:189–199
Hall JL, Ye J, Diddams SA, Ma L-S, Cundiff ST, Jones DJ(2001) Ultrasensitive spectroscopy, the ultrastable lasers, theultrafast lasers, and the seriously nonlinear fiber: a new alliancefor physics and metrology. IEEE J Quantum Electron 37:1482–1492
Holzwarth R, Zimmermann M, Udem T, Hänsch TW (2001)Optical clockworks and the measurement of laser frequencies witha mode-locked frequency comb. IEEE J Quantum Electron 37:1493–1501
Cundiff ST, Ye J (2003) Femtosecond optical frequencycombs. Rev Modern Phys 75:325–342
Helbing FW, Steinmeyer G, Stenger J, Telle HR, Keller U(2002) Carrier-envelope-offset dynamics and stabilization offemtosecond pulses. Appl Phys B 74:S34–S42
Ranka J, Windeler R, Stentz A (2000) Visible continuumgeneration in air-silica microstructure optical fibers with anomalousdispersion at 800 nm. Opt Lett 25:25–27
Ranka JK, Windeler RS, Stentz AJ (2000) Opticalproperties of high-delta air silica microstructure optical fibers. OptLett 25:796–798
Xu L, Spielmann C, Poppe A, Brabec T, Krausz F, HänschTW (1996) Route to phase control of ultrashort light pulses. Opt Lett21:2008–2010
Matos L, Mücke OD, Jian C, Kärtner FX (2006)Carrier-envelope phase dynamics and noise analysis inoctave-spanning Ti:sapphire lasers. Opt Express 14:2497–2511
Stenger J, Talle HR (2000) Intensity-induced modeshift in a femtosecond laser by a change in the nonlinear index ofrefraction. Opt Lett 25:1553–1555
Holman KW, Jones RJ, Marian A, Cundiff ST, Ye J (2003)Detailed studies and control of intensity related dynamics offemtosecond frequency combs from mode-locked Ti-sapphirelasers. IEEE J Select Topics Quantum Electron 9:1018
Kutz JN (1998) Modelocking pulse dynamics in fiberlasers. In: SPIE Conference on Physics and Simulation ofOptoelectronics Devices VI, vol 3283, (San Jose, CA). SPIE,pp 639–651
Washburn BR, Swan WC, Newberry NR (2005) Responsedynamics of the frequency comb output from a femtosecond fiberlaser. Opt Lett 13:10622–10633
Cundiff ST (2005) Soliton dynamics in mode-lockedlasers. Lecture notes in physics, vol 661. Springer, Berlin, pp 183–206
Acknowledgments
The author is greatly indebted to many colleagues, friends andteachers who have influenced me over the years. I wish to thankDr. Steven T. Cundiff and Professor Curtis R. Menyuk for theirtremendous contributions and stimulating conversations regardingtheir recent efforts in understanding this vast field. To Dr. JohnL. Hall I owe a great and hearty thanks for all of his pioneeringwork, for his patience as a sounding board and his uniqueperspective on physics. Thanks also to Professors AnthonyE. Siegman, Stephen E. Harris, Robert L. Byer, and especially, Alwyn C. Scott, from whom I learned much. Finally, on behalf of my groupat the University of California, I wish to thank Robert Temple, TomFaulkner and Roger Muat of Agilent Technologies (formerlyHewlett-Packard Company) for numerous donations and countless hoursof tutoring.
This work was supported in part by the David and Lucile PackardFoundation and the National Science Foundation under grantECS-0622235.
Author information
Authors and Affiliations
Editor information
Editors and Affiliations
Rights and permissions
Copyright information
© 2009 Springer-Verlag
About this entry
Cite this entry
Kolner, B.H. (2009). Noise and Stability in Modelocked Soliton Lasers. In: Meyers, R. (eds) Encyclopedia of Complexity and Systems Science. Springer, New York, NY. https://doi.org/10.1007/978-0-387-30440-3_360
Download citation
DOI: https://doi.org/10.1007/978-0-387-30440-3_360
Publisher Name: Springer, New York, NY
Print ISBN: 978-0-387-75888-6
Online ISBN: 978-0-387-30440-3
eBook Packages: Physics and AstronomyReference Module Physical and Materials ScienceReference Module Chemistry, Materials and Physics