Delayed Feedback Versus Seasonal Forcing: Resonance Phenomena in an El Nin͂o Southern Oscillation Model

Climate models can take many different forms, from very detailed highly computational models with hundreds of thousands of variables, to more phenomenological models of only a few variables that are designed to investigate fundamental relationships in the climate system. Important ingredients in these models are the periodic forcing by the seasons, as well as global transport phenomena of quantities such as air or ocean temperature and salinity. We consider a phenomenological model for the El Nino Southern Oscillation system, where the delayed effects of oceanic waves are incorporated explicitly into the model. This gives a description by a delay differential equation, which models underlying fundamental processes of the interaction between internal delay-induced oscillations and the external forcing. The combination of delay and forcing in differential equations has also found application in other fields, such as ecology and gene networks. Specifically, we present exemplary stable solutions of the model...

[1]  Roger D. Nussbaum,et al.  Uniqueness and nonuniqueness for periodic solutions of x′(t) = −g(x(t − 1)) , 1979 .

[2]  D. Roose,et al.  Continuation and Bifurcation Analysis of Delay Differential Equations , 2007 .

[3]  Raymond T. Pierrehumbert,et al.  Bifurcations leading to summer Arctic sea ice loss , 2011 .

[4]  H. Broer,et al.  Quasi-Periodicity in Dissipative and Conservative Systems , 2005 .

[5]  Daan Lenstra,et al.  Theory of delayed optical feedback in lasers , 2000 .

[6]  Neville Nicholls,et al.  Is there an Indian Ocean dipole and is it independent of the El Niño-Southern Oscillation? , 2001 .

[7]  Francis H. S. Chiew,et al.  El Niño/Southern Oscillation and Australian rainfall and streamflow , 2003 .

[8]  Fei-Fei Jin,et al.  An Equatorial Ocean Recharge Paradigm for ENSO. Part I: Conceptual Model , 1997 .

[9]  Mark A. Cane,et al.  A study of self-excited oscillations of the tropical ocean-atmosphere system , 1990 .

[10]  Yulin Cao,et al.  Uniqueness of Periodic Solution for Differential Delay Equations , 1996 .

[11]  By,et al.  Some simple solutions for heat-induced tropical circulation , 2006 .

[12]  Peter Cox,et al.  Tipping points in open systems: bifurcation, noise-induced and rate-dependent examples in the climate system , 2011, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[13]  Hendrik Broer,et al.  Quasi-periodic bifurcations of invariant circles in low-dimensional dissipative dynamical systems , 2011 .

[14]  Steven H. Strogatz,et al.  Nonlinear Dynamics and Chaos , 2024 .

[15]  Ken Kiyono,et al.  Bifurcations Induced by Periodic Forcing and Taming Chaos in Dripping Faucets , 2002 .

[16]  Cristina Masoller,et al.  Experimental and numerical study of the symbolic dynamics of a modulated external-cavity semiconductor laser. , 2014, Optics express.

[17]  H. Knolle,et al.  Lotka-volterra equations with time delay and periodic forcing term , 1976 .

[18]  Hil Meijer,et al.  Numerical Bifurcation Analysis , 2009, Encyclopedia of Complexity and Systems Science.

[19]  Allan J. Clarke,et al.  Improving El Niño prediction using a space‐time integration of Indo‐Pacific winds and equatorial Pacific upper ocean heat content , 2003 .

[20]  Warden,et al.  Locking and Arnold tongues in an infinite-dimensional system: The nuclear magnetic resonance laser with delayed feedback. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[21]  Michael Ghil,et al.  A delay differential model of ENSO variability – Part 2: Phase locking, multiple solutions and dynamics of extrema , 2010, 1003.0028.

[22]  Michael Ghil,et al.  El Ni�o on the Devil's Staircase: Annual Subharmonic Steps to Chaos , 1994, Science.

[23]  Eli Tziperman,et al.  Locking of El Nino's Peak Time to the End of the Calendar Year in the Delayed Oscillator Picture of ENSO , 1998 .

[24]  Zengrong Liu,et al.  Periodic oscillation in delayed gene networks with SUM regulatory logic and small perturbations. , 2009, Mathematical biosciences.

[25]  Robert S. MacKay,et al.  Resonances for weak coupling of the unfolding of a saddle-node periodic orbit with an oscillator , 2007 .

[26]  W. H. Quinn,et al.  HISTORICAL TRENDS AND STATISTICS OF THE SOUTHERN OSCILLATION, EL NINO, AND INDONESIAN DROUGHTS , 1978 .

[27]  Bernd Krauskopf,et al.  Bifurcation analysis of delay-induced resonances of the El-Niño Southern Oscillation , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[28]  S Yanchuk,et al.  Delay and periodicity. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[29]  Y. N. Kyrychko,et al.  Global properties of a delayed SIR model with temporary immunity and nonlinear incidence rate , 2005 .

[30]  Michael Ghil,et al.  Solving problems with GCMs: General circulation models and their role in the climate modeling hierarchy , 2000 .

[31]  Philipp Hövel,et al.  Clustering in delay-coupled smooth and relaxational chemical oscillators. , 2013, Physical review. E, Statistical, nonlinear, and soft matter physics.

[32]  L. Shampine,et al.  Solving DDEs in MATLAB , 2001 .

[33]  T. McMahon,et al.  El Nino/Southern Oscillation and Australian rainfall, streamflow and drought : Links and potential for forecasting , 1998 .

[34]  Hans Kaper,et al.  Mathematics and Climate , 2013 .

[35]  Jong-Seong Kug,et al.  The impacts of the model assimilated wind stress data in the initialization of an intermediate ocean and the ENSO predictability , 2001 .

[36]  J. Michael T. Thompson,et al.  Predicting Climate tipping as a Noisy bifurcation: a Review , 2011, Int. J. Bifurc. Chaos.

[37]  Philipp Hövel,et al.  Time-delayed feedback in neurosystems , 2008, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[38]  Michael Ghil,et al.  A delay differential model of ENSO variability: parametric instability and the distribution of extremes , 2007, 0712.1312.

[39]  A. Barnston,et al.  Prediction of ENSO Episodes Using Canonical Correlation Analysis , 1992 .

[40]  Eli Tziperman,et al.  El Ni�o Chaos: Overlapping of Resonances Between the Seasonal Cycle and the Pacific Ocean-Atmosphere Oscillator , 1994, Science.

[41]  Claire M Postlethwaite,et al.  Stabilizing unstable periodic orbits in the Lorenz equations using time-delayed feedback control. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[42]  Richard McGehee,et al.  Resonance Surfaces for Forced Oscillators , 1994, Exp. Math..

[43]  Giovanni Samaey,et al.  DDE-BIFTOOL Manual - Bifurcation analysis of delay differential equations , 2014, 1406.7144.

[44]  Y. Kuznetsov Elements of Applied Bifurcation Theory , 2023, Applied Mathematical Sciences.

[45]  D. Enfield,et al.  Tropical Atlantic sea surface temperature variability and its relation to El Niño‐Southern Oscillation , 1997 .

[46]  D. Aronson,et al.  Bifurcations from an invariant circle for two-parameter families of maps of the plane: A computer-assisted study , 1982 .

[47]  Glass,et al.  Periodic forcing of a limit-cycle oscillator: Fixed points, Arnold tongues, and the global organization of bifurcations. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[48]  Geert Jan van Oldenborgh,et al.  The Relationship between Sea Surface Temperature and Thermocline Depth in the Eastern Equatorial Pacific , 2004 .

[49]  Eli Tziperman,et al.  Irregularity and Locking to the Seasonal Cycle in an ENSO Prediction Model as Explained by the Quasi-Periodicity Route to Chaos , 1995 .

[50]  Shui-Nee Chow,et al.  Characteristic multipliers and stability of symmetric periodic solutions of x'(t)=g(x(t−1)) , 1988 .

[51]  Kestutis Pyragas Continuous control of chaos by self-controlling feedback , 1992 .

[52]  Mark A. Cane,et al.  Experimental forecasts of El Niño , 1986, Nature.

[53]  Alexey Kaplan,et al.  Predictability of El Niño over the past 148 years , 2004, Nature.

[54]  S. Saha,et al.  The NCEP Climate Forecast System , 2006 .

[55]  Masayoshi Inoue,et al.  Scenarios Leading to Chaos in a Forced Lotka-Volterra Model , 1984 .

[56]  Max J. Suarez,et al.  Vacillations in a Coupled Ocean–Atmosphere Model , 1988 .

[57]  Allan J. Clarke,et al.  An Introduction to the Dynamics of El Nino and the Southern Oscillation , 2008 .

[58]  Jong-Seong Kug,et al.  An El‐Nino Prediction System using an intermediate ocean and a statistical atmosphere , 2000 .

[59]  Bernd Krauskopf,et al.  Bifurcation Analysis of Lasers with Delay , 2003 .

[60]  K Aihara,et al.  Periodic and non-periodic responses of a periodically forced Hodgkin-Huxley oscillator. , 1984, Journal of theoretical biology.

[61]  Fei-Fei Jin,et al.  An Equatorial Ocean Recharge Paradigm for ENSO. Part II: A Stripped-Down Coupled Model , 1997 .

[62]  Bin Wang,et al.  Interactions between the Seasonal Cycle and El Niño-Southern Oscillation in an Intermediate Coupled Ocean-Atmosphere Model , 1995 .

[63]  Kanehiro Kitayama,et al.  Effects of the 1997–98 El Niño drought on rain forests of Mount Kinabalu, Borneo , 2002, Journal of Tropical Ecology.

[64]  J. Bjerknes,et al.  ATMOSPHERIC TELECONNECTIONS FROM THE , 2004 .

[65]  Max J. Suarez,et al.  A Delayed Action Oscillator for ENSO , 1988 .