2007
DOI: 10.1016/j.automatica.2007.03.013
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Representations and structural properties of periodic systems

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Cited by 14 publications
(15 citation statements)
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“…On the other hand, ℓ can clearly be reconstructed from w 1 =2ℓ and w 2 =3ℓ. Similar phenomena can also be observed with periodic systems 16, and have already been reported for systems over rings in 17.…”
Section: Controllabilitysupporting
confidence: 83%
“…On the other hand, ℓ can clearly be reconstructed from w 1 =2ℓ and w 2 =3ℓ. Similar phenomena can also be observed with periodic systems 16, and have already been reported for systems over rings in 17.…”
Section: Controllabilitysupporting
confidence: 83%
“…If F is a field, N = Z ⊃ L = Zn and B ⊂ W N × is a closed subspace the invariance means q n • B = B. This is the case treated in Kuijper and Willems (1997) and Aleixo et al (2007a).…”
Section: Relation To Previous Workmentioning
confidence: 96%
“…The main results of this paper described above are contained in Sections 5 and 6. Section 3 describes the module-behavior duality for periodic behaviors on the time-axis N. For the time-axis Z the theory is simpler and was treated with similar methods in [5] where we also explained the relation with previous work [11], [1], [2]. In Section 4 we apply Morita theory to derive essential notions for and properties of periodic behaviors and their dual f.g. B-left modules, for instance autonomy, controllability, the existence and characterization of input/output (IO) structures and left and right coprime factorizations.…”
Section: ]mentioning
confidence: 99%
“…They solve open problems that were raised in [1, §7]. In contrast to [11], [1] and [5] and in accordance with [9], [2] and [16] (in the LTI case) we consider N -periodic systems on the time-axis N ∋ t of natural numbers and not on Z. A periodic system is a linear time-varying (LTV) system whose coefficient functions a are N -periodic, i.e., satisfy a(t + N ) = a(t) for t ∈ N. If F denotes any field or, in Sections 5 and 6, the field R or C of real or complex numbers, the coefficient functions form the commutative algebra F Z/ZN of functions from Z/ZN to F where we pose a(t) := a(t + ZN ) for t ∈ N. The monoid N acts on a ∈ F Z/ZN via algebra isomorphisms by (j • a)(t + ZN ) := a(j + t + ZN ).…”
Section: Introductionmentioning
confidence: 99%