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All periodic time scales are unbounded above and below.
All periodic displacement configurations which minimize the bottom of the spectrum are characterized.
All periodic time scales are particular changing-periodic time scales and complete.
All periodic data packets include three fields specified in the ADV packet.
All periodic patterns such that (p=1) are included in a group (mathcal {P}_T^1), all periodic patterns such that (p=2) are included in a group (mathcal {P}_T^2),...all periodic patterns such that (p~mathrm{mod}~f = 0) where (f) is a prime number are included in a group (mathcal {P}_T^f).
(1.2) In [23], the authors considered the case that the coefficients of (1.2) are all periodic functions with period T. They obtained the stochastic permanence of (1.2) and global attractivity of one positive solution (x^{p}(t)) satisfying (mathrm{E}[1/x^{p}(t)]=mathrm{E}[1/x^{p}(t+T ]).
The coefficients of model (3.2) are all periodic with the common period 20.
So, (S^), (S^), and L are all periodic sets with the period aπ, where S^=bigcup_{k=-infty}^{+infty}S^_{k}.
We will further investigate the existence and stability of the periodic solution for model (1.1) under the assumption that the coefficients of model (1.1) are all periodic with a common period.
for all periodic solutions y(n) of period p of the adjoint Equation (7).
Suppose that (42) is satisfied for all periodic solutions y(n) of period p of (7).
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