Sparse identification of a predator-prey system from simulation data of a convection model
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Jan S. Hesthaven | J. Juul Rasmussen | Volker Naulin | Morten Brøns | Magnus Dam | J. Hesthaven | M. Brøns | J. Rasmussen | V. Naulin | M. Dam
[1] S. Chapman,et al. Transitions to improved confinement regimes induced by changes in heating in zero-dimensional models for tokamak plasmas , 2014 .
[2] Metamorphosis of plasma turbulence-shear-flow dynamics through a transcritical bifurcation. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.
[3] W. Fundamenski,et al. Radial interchange motions of plasma filaments , 2006 .
[4] Wen-Xu Wang,et al. Predicting catastrophes in nonlinear dynamical systems by compressive sensing. , 2011, Physical review letters.
[5] Lennart Ljung,et al. System identification (2nd ed.): theory for the user , 1999 .
[6] W. Fundamenski,et al. Interchange turbulence in the TCV scrape-off layer , 2006 .
[7] B. Wan,et al. One-dimensional modelling of limit-cycle oscillation and H-mode power scaling , 2015 .
[8] Steven L. Brunton,et al. Inferring Biological Networks by Sparse Identification of Nonlinear Dynamics , 2016, IEEE Transactions on Molecular, Biological and Multi-Scale Communications.
[9] P. Diamond,et al. Study of the L–I–H transition with a new dual gas puff imaging system in the EAST superconducting tokamak , 2013 .
[10] S. Chapman,et al. Robustness of predator-prey models for confinement regime transitions in fusion plasmas , 2013, 1302.0727.
[11] J. Madsen,et al. Simulation of transition dynamics to high confinement in fusion plasmas , 2014, 1409.3186.
[12] Suppression of turbulence at low power input in a model for plasma confinement transitions , 2005 .
[13] F. Wagner,et al. A quarter-century of H-mode studies , 2007 .
[14] P. Diamond,et al. Direct identification of predator-prey dynamics in gyrokinetic simulations , 2015 .
[15] Edward A. Spiegel,et al. Rayleigh‐Bénard Convection: Structures and Dynamics , 1998 .
[16] S. Benkadda,et al. Confinement and bursty transport in a flux-driven convection model with sheared flows , 2003 .
[17] Lennart Ljung,et al. System Identification: Theory for the User , 1987 .
[18] Ö. Gürcan,et al. Characterization of predator–prey dynamics, using the evolution of free energy in plasma turbulence , 2012, 1205.5712.
[19] W. Horton,et al. L-h confinement mode dynamics in three-dimensional state space , 1995 .
[20] P. Diamond,et al. Weak hysteresis in a simplified model of the L-H transition , 2009 .
[21] Urbashi Mitra,et al. Editorial: Inaugural Issue of the IEEE Transactions on Molecular, Biological, and Multi-Scale Communications , 2015, IEEE Trans. Mol. Biol. Multi Scale Commun..
[22] X. Garbet,et al. The quasilinear behavior of convective turbulence with sheared flows , 2003 .
[23] P. Diamond,et al. Zonal flows and pattern formation , 2015 .
[24] O. E. Garcia,et al. Mechanism and scaling for convection of isolated structures in nonuniformly magnetized plasmas , 2005 .
[25] J. Rasmussen,et al. Numerical modeling of the transition from low to high confinement in magnetically confined plasma , 2015 .
[26] P. Diamond,et al. Mean shear flows, zonal flows, and generalized Kelvin–Helmholtz modes in drift wave turbulence: A minimal model for L→H transition , 2003 .
[27] Ö. Gürcan,et al. Spatio-temporal evolution of the L → I → H transition , 2012 .
[28] O. E. Garcia,et al. Structures, profile consistency, and transport scaling in electrostatic convection , 2005 .
[29] S. Brunton,et al. Discovering governing equations from data by sparse identification of nonlinear dynamical systems , 2015, Proceedings of the National Academy of Sciences.
[30] M. Brøns,et al. Bifurcation analysis and dimension reduction of a predator-prey model for the L-H transition , 2013 .
[31] J. Juul Rasmussen,et al. Turbulence and intermittent transport at the boundary of magnetized plasmas , 2005 .