A model for oscillations and pattern formation in protoplasmic droplets of Physarum polycephalum
暂无分享,去创建一个
[1] R. Rivlin. Large elastic deformations of isotropic materials IV. further developments of the general theory , 1948, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.
[2] T. Ueda,et al. Propagation of phase wave in relation to tactic responses by the plasmodium of Physarum polycephalum , 1986 .
[3] Yonosuke Kobatake,et al. Phototaxis in true slime mold Physarum polycephalum , 1976 .
[4] A. Tero,et al. A coupled-oscillator model with a conservation law for the rhythmic amoeboid movements of plasmodial slime molds , 2005 .
[5] G. Odell,et al. Mechanics of cytogels I: oscillations in physarum. , 1984, Cell motility.
[6] K Kurihara,et al. Chemotaxis in Physarum polycephalum. Effects of chemicals on isometric tension of the plasmodial strand in relation to chemotactic movement. , 1976, Experimental cell research.
[7] P K Maini,et al. Dispersion relation in oscillatory reaction-diffusion systems with self-consistent flow in true slime mold , 2007, Journal of mathematical biology.
[8] V. A. Teplov,et al. A continuum model of contraction waves and protoplasm streaming in strands of Physarum plasmodium. , 1991, Bio Systems.
[9] T. Ueda,et al. Interaction between cell shape and contraction pattern in the Physarum plasmodium. , 2000, Biophysical chemistry.
[10] T. Ueda,et al. Reversal of thermotaxis with oscillatory stimulation in the plasmodium of Physarum polycephalum , 1988 .
[11] N. Kamiya. Contractile Properties of the Plasmodial Strand , 1970 .
[12] A. Tero,et al. Rules for Biologically Inspired Adaptive Network Design , 2010, Science.
[13] J. Butcher. Numerical Methods for Ordinary Differential Equations: Butcher/Numerical Methods , 2005 .
[14] Einar M. Rønquist,et al. An Operator-integration-factor splitting method for time-dependent problems: Application to incompressible fluid flow , 1990 .
[15] Seiji Takagi,et al. Annihilation and creation of rotating waves by a local light pulse in a protoplasmic droplet of the Physarum plasmodium , 2010 .
[16] D. Smith,et al. Model of the Ca2+ oscillator for shuttle streaming in Physarum polycephalum. , 1992, Biophysical journal.
[17] Dan Luss,et al. Impact of global interaction on pattern formation on a disk , 1995 .
[18] George Oster,et al. The mechanochemistry of cytogels , 1984 .
[19] J. Butcher. Numerical methods for ordinary differential equations , 2003 .
[20] T. Nakagaki,et al. Intelligent Behaviors of Amoeboid Movement Based on Complex Dynamics of Soft Matter , 2007 .
[21] Werner Baumgarten,et al. Plasmodial vein networks of the slime mold Physarum polycephalum form regular graphs. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.
[22] Jonathan Richard Shewchuk,et al. Delaunay refinement algorithms for triangular mesh generation , 2002, Comput. Geom..
[23] Nakagaki,et al. Reaction-diffusion-advection model for pattern formation of rhythmic contraction in a giant amoeboid cell of the physarum plasmodium , 1999, Journal of theoretical biology.
[24] J. Shewchuk. An Introduction to the Conjugate Gradient Method Without the Agonizing Pain , 1994 .
[25] M P Nash,et al. Drift and breakup of spiral waves in reaction–diffusion–mechanics systems , 2007, Proceedings of the National Academy of Sciences.
[26] T. Ueda,et al. Emergence and transitions of dynamic patterns of thickness oscillation of the plasmodium of the true slime mold Physarum polycephalum , 2008 .
[27] A. Tero,et al. Mathematical Model for Rhythmic Protoplasmic Movement in the True Slime Mold , 2006, Journal of mathematical biology.
[28] Robert D. Allen,et al. Shuttle-Streaming: Synchronization with Heat Production in Slime Mold , 1963, Science.
[29] S. Takagi,et al. Locomotive mechanism of Physarum plasmodia based on spatiotemporal analysis of protoplasmic streaming. , 2008, Biophysical journal.
[30] A F Mak,et al. The apparent viscoelastic behavior of articular cartilage--the contributions from the intrinsic matrix viscoelasticity and interstitial fluid flows. , 1986, Journal of biomechanical engineering.
[31] E. Alvarez-Lacalle,et al. Global coupling in excitable media provides a simplified description of mechanoelectrical feedback in cardiac tissue. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.
[32] T. Nakagaki,et al. Pattern formation of a reaction-diffusion system with self-consistent flow in the amoeboid organism Physarum plasmodium , 1998, patt-sol/9805004.
[33] W Alt,et al. Cytoplasm dynamics and cell motion: two-phase flow models. , 1999, Mathematical biosciences.
[34] H. Engel,et al. Chemical turbulence and standing waves in a surface reaction model: The influence of global coupling and wave instabilities. , 1994, Chaos.
[35] Alexander S. Mikhailov,et al. Turbulence and standing waves in oscillatory chemical reactions with global coupling , 1994 .
[36] N. Kamiya,et al. Torsion in a protoplasmic thread. , 1954, Experimental cell research.