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5544290817
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note
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This type of control can also be written in terms of a sequence of Dirac pulses, and can easily be implemented electronically using sampling circuits; see [21].
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32
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0000794185
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For the proof of the theorem, see T. Stojanovski, L. Kocarev, U. Parlitz, and R. Harris, Phys. Rev. E 55, 4035 (1997).
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85088809633
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note
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v) decomposition, one can always turn to two or more dimensional controlling sequences.
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34
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0346644912
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K. Kaneko, Physica D 24, 1 (1989); 41, 137 (1990).
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85088809574
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note
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L=34.
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38
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5544282377
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note
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The initial conditions for the periodic orbit used in the simulations are x(0) = 1.171 139 297 806 379, y(0) = 1.627059 584 491 594 and z(0) = 15.298 955 084 754 981.
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40
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5544243009
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note
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The initial conditions for the first unstable periodic orbit are given in [28], while for the other orbit they are: x(0) = 4.560 295 060 061 776, y(0) = 6.260 735 588 766 367, and z(0) = 16.709 465 601 707 183.
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