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Dynamical Systems in Neuroscience:

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218 Bifurcationsbifurcationssaddle-nodesaddle-node on <strong>in</strong>variant cicleAndronov-Hopfsaddle homocl<strong>in</strong>ic orbitfold limit cyclesaddle-node homocl<strong>in</strong>ic orbitBogdanov-TakensBaut<strong>in</strong>flipalternative namesfold, limit po<strong>in</strong>t, saddle-node off limit cycleSNIC, saddle-node on limit cycle (SNLC), circle,saddle-node homocl<strong>in</strong>ic, saddle-node central homocl<strong>in</strong>ic,saddle-node <strong>in</strong>f<strong>in</strong>ite period (SNIPer), homocl<strong>in</strong>icHopf, Po<strong>in</strong>care-Andronov-Hopfhomocl<strong>in</strong>ic, saddle-loop, saddle separatrix loop, Andronov-Leontovichsaddle-node of limit cycles, double limit cycle, fold cycle,saddle-node (fold) of periodicssaddle-node noncentral homocl<strong>in</strong>ic, saddle-node separatrix-loopTakens-Bogdanov, double-zerodegenerate Hopf, generalized Hopfperiod doubl<strong>in</strong>gFigure 6.49: Popular alternative names to some of the bifurcations considered <strong>in</strong> thischapter.science. More bifurcation theory, <strong>in</strong>clud<strong>in</strong>g bifurcations <strong>in</strong> mapp<strong>in</strong>gs x n+1 = f(x n , b),can be found <strong>in</strong> the excellent book “Elements of Applied Bifurcation Theory” by YuriKuznetsov (1995, new edition 2004), which, however, might be a bit technical fora non-mathematician. Some of the bifurcations considered <strong>in</strong> this chapter, such asthe blue-sky catastrophe, are classified as “exotic” by Kuznetsov (1995), though thecatastrophe was recently found <strong>in</strong> a model of a leech heart <strong>in</strong>terneuron (Shilnikov andCymbalyuk 2005).There is no unified nam<strong>in</strong>g scheme for the bifurcations, mostly because they werediscovered and rediscovered <strong>in</strong>dependently <strong>in</strong> many fields and <strong>in</strong> many countries. Forexample, the Andronov-Hopf bifurcation was known to Po<strong>in</strong>care, so some scientistsrefer to it as Po<strong>in</strong>care-Andronov-Hopf bifurcation. Many refer to it as just Hopf bifurcationdue to the fault of no lesser men than the famous Russian mathematicianVladimir Igorevich Arnold and famous French mathematician Rene Thom. Accord<strong>in</strong>gto Arnold’s own accounts, he was visited by Thom <strong>in</strong> the 1960s. While discuss<strong>in</strong>g variousbifurcations, Arnold put too much emphasis on the “recent” Hopf (1942) paper.As a result of Arnold’s misattribution, Thom popularized the bifurcation as be<strong>in</strong>g Hopfbifurcation. In Fig. 6.49 we provide some common alternative names to the bifurcationsconsidered <strong>in</strong> this chapter. The complete list of names of known bifurcations is toolong, and it resembles the list of faculty members of the department of RadioPhysics(Gorky State University, now Nizhnii Novgorod, Russia) founded by A.A. Andronov<strong>in</strong> 1945.The division of bifurcations <strong>in</strong>to subcritical and supercritical ones may be confus<strong>in</strong>gfor a novice. For example, some scientists erroneously th<strong>in</strong>k that supercritical bifurcationsresult <strong>in</strong> appearance of attractors (stable equilibria, limit cycles, etc.) andsubcritical bifurcations result <strong>in</strong> their disappearance. Let us emphasize here that theappearance or disappearance of an equilibrium or a limit cycle depends on the directionof change of the bifurcation parameter. For example, the subcritical pitchfork

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