Impulse pattern in bi-directionally coupled model neurons of different dynamics

The effects of bi-directional gap junction coupling of two model neurons with subthreshold oscillations have been examined when the individual neurons are operating at different dynamical states either in the tonic or bursting firing mode. Our simulations indicate that intermediate coupling strengths mostly lead to highly variable, often chaotic impulse patterns whereas transition to completely synchronized activity at high coupling strengths is generally going along with transitions to regular limit cycle activity. The synchronized activity pattern, however, can be completely different from the original pattern of the uncoupled neurons.

[1]  H A Braun,et al.  Stimulus sensitivity and neuromodulatory properties of noisy intrinsic neuronal oscillators. , 1998, Bio Systems.

[2]  Teresa Ree Chay,et al.  Electrical bursting and intracellular Ca2+ oscillations in excitable cell models , 1990, Biological Cybernetics.

[3]  H A Braun,et al.  Phase-space structure of a thermoreceptor. , 2000, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[4]  Hans A Braun,et al.  Oscillations, resonances and noise: basis of flexible neuronal pattern generation. , 2003, Bio Systems.

[5]  R. Dyball,et al.  Phasic firing enhances vasopressin release from the rat neurohypophysis , 1979, The Journal of physiology.

[6]  H. Braun,et al.  Interactions of temperature and angiotensin II in paraventricular neurons of rats in vitro , 2002, Pflügers Archiv.

[7]  Andrey Shilnikov,et al.  Mechanism of bistability: tonic spiking and bursting in a neuron model. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.

[8]  W. Singer,et al.  Stimulus-specific neuronal oscillations in orientation columns of cat visual cortex. , 1989, Proceedings of the National Academy of Sciences of the United States of America.

[9]  G. Dayanithi,et al.  The role of patterned burst and interburst interval on the excitation‐coupling mechanism in the isolated rat neural lobe. , 1985, The Journal of physiology.

[10]  Young Seek Lee,et al.  Bursting, Beating, and Chaos by Two Functionally Distinct Inward Current Inactivations in Excitable Cells a , 1990 .

[11]  Fabrizio Gabbiani,et al.  Burst firing in sensory systems , 2004, Nature Reviews Neuroscience.

[12]  Erik Mosekilde,et al.  INTER-PATTERN TRANSITIONS IN A NOISY BURSTING CELL , 2004 .

[13]  A. Hodgkin,et al.  A quantitative description of membrane current and its application to conduction and excitation in nerve , 1990 .

[14]  Frank Moss,et al.  Homoclinic bifurcation in a Hodgkin-Huxley model of thermally sensitive neurons. , 2000, Chaos.

[15]  F Moss,et al.  Stochastic phase synchronization in the crayfish mechanoreceptor/photoreceptor system. , 2003, Chaos.

[16]  David A. McCormick,et al.  Are thalamocortical rhythms the rosetta stone of a subset of neurological disorders? , 1999, Nature Medicine.

[17]  F Moss,et al.  Noise-induced impulse pattern modifications at different dynamical period-one situations in a computer model of temperature encoding. , 2001, Bio Systems.

[18]  Sonya Bahar BURST-ENHANCED SYNCHRONIZATION IN AN ARRAY OF NOISY COUPLED NEURONS , 2004 .