A model of a hard oscillator with analytic solution is presented. Its behavior under periodic kicking, for which a closed form stroboscopic map can be obtained, is studied. It is shown that the general structure of such an oscillator includes four distinct regions; the outer two regions correspond to very small or very large amplitude of the external force and match the corresponding regions in soft oscillators (invertible degree one and degree zero circle maps, respectively). There are two new regions for intermediate amplitude of the forcing. Region 3 corresponds to moderate high forcing, and is intrinsic to hard oscillators; it is characterized by discontinuous circle maps with a flat segment. Region 2 (low moderate forcing) has a certain resemblance to a similar region in soft oscillators (noninvertible degree one circle maps); however, the limit set of the dynamics in this region is not a circle, but a branched manifold, obtained as the tangent union of a circle and an interval; the topological structure of this object is generated by the finite size of the repelling set, and is therefore also intrinsic to hard oscillators.  

1.
M.
Guevara
and
L.
Glass
,
J. Math. Biol.
14
,
1
(
1982
).
2.
L.
Glass
and
R.
Perez
,
Phys. Rev. Lett.
48
,
1772
(
1982
).
3.
D. L.
Gonzalez
and
O.
Piro
,
Phys. Rev. Lett.
50
,
12
(
1983
).
4.
L.
Glass
,
M.
Guevara
,
A.
Shrier
, and
R.
Perez
,
Physica D
7
,
89
(
1983
).
5.
T.
Allen
, IEEE Trans. Circ. Sys, Sept. 1983. See also T. Allen,
Physica D
6
,
305
(
1983
).
6.
L.
Glass
and
A. T.
Winfree
,
Am. J. Physiol.
246
,
R251
(
1984
).
7.
D. L.
Gonzalez
and
O.
Piro
,
Phys. Lett. A
101
,
9
(
1984
).
8.
J. P.
Keener
and
L.
Glass
,
J. Math. Biol.
21
,
175
(
1984
).
9.
R. S.
Mackay
and
C.
Tresser
,
Physica D
19
,
206
(
1986
).
10.
E. J.
Ding
,
Phys. Rev. A
35
,
2669
(
1987
).
11.
L. Glass and M. Mackey, From Clocks to Chaos (Princeton University, Princeton, NJ, 1988).
12.
J. L.
McCauley
,
Physica Scripta T
20
,
34
(
1988
), and references therein.
13.
A.
Campbell
,
A.
Gonzales
,
D. L.
Gonzalez
,
O.
Piro
, and
H. A.
Larrondo
,
Physica A
155
,
565
(
1989
).
14.
L.
Glass
and
P.
Hunter
,
Physica D
43
,
1
(
1990
).
15.
Q.
Tong
and
Z.
Liu
,
Int. J. Cardiol.
26
,
211
(
1990
).
16.
W. Z.
Zeng
,
M.
Courtemanche
,
L.
Sehn
,
A.
Shrier
, and
L.
Glass
,
J. Theor. Biol.
145
,
254
(
1990
).
17.
N. Minorsky, Nonlinear Oscillations (Van Nostrand, Princeton, 1962).
18.
V. M. Starzhinskii, Applied methods in the theory of nonlinear oscillations (Mir, Moscow, 1980).
19.
R.
Mackay
,
Physica D
52
,
254
(
1991
).
20.
D. Ruelle, Elements of differentiable dynamics and bifurcation theory (Academic, Boston, 1989).
21.
J. Guckenheimer and P. Holmes, Nonlinear Oscillations, Dynamical Systems, and Bifurcations of Vector Fields (Springer-Verlag, Berlin, 1983).
22.
Jacob Palis and Welington de Melo, Introducao aos Sistemas Dinamicos (IMPA Projeto Euclides, Rio do Janeiro, 1985).
23.
Michael Shub, Global Stability of Dynamical Systems (Springer, New York, 1988).
24.
Strictly speaking one must allow for an odd number of intersections of the limit cycle with the vertical downwards ray starting at the fixed point, therefore defining an odd number of critical lines and a number of sub- and supracritical regions; such oscillators, however, cannot be realized as second-order odes in one degree of freedom, and are not small perturbations thereof, therefore excluding most electronic and electromechanical oscillators.
25.
The topological degree of a map of the circle is defined as
and represents the number of times the function winds around the circle as the argument winds once.
26.
In addition, if Fe < re, we will observe an extra stable limit set, since an initial condition inside the unstable limit cycle will be trapped inside if Fe is small enough and μ and τ are large enough. There is therefore an extra attracting set for some parameter values.
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