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Design of Seasonal Adjustment Filter Robust to Variations in the Seasonal Behaviour of Time Series

.” Journal of the Royal Statistical Society: Series A (General) 143: 321-337. Doi: http://dx.doi.org/10.2307/2982132. Canova, F. and E. Ghysels. 1994. “Changes in Seasonal Patterns: Are They Cyclical?” Journal of Economic Dynamics and Control 18: 1143-1171. Available at: http://apps.eui.eu/Personal/Canova/Articles/chanseapat.pdf (accessed September 2015). Canova, F. and B.E. Hansen. 1995. “Are Seasonal Patterns Constant Over Time? A Test for Seasonal Stability.” Journal of Business & Economic Statistics 13: 237-252. Doi: http://dx.doi.org/10

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Questions Around the Thue-Morse Sequence

applications to Riesz products. Proc. Amer. Math. Soc. 131 (2003), 165–174. [18] HOST, B.: Nombres normaux, entropie, translations , Israel J. Math. 91 (1995), no. 1–3, 419–428. [19] KAMAE, T.: Cyclic extensions of odometer transformations and spectral disjointness , Israel J. Math. 59 (1987), 41–63. [20] KAMAE, T.: Number-theoretic problems involving two independent bases . In: Number theory and cryptography (Sydney, 1989), London Math. Soc. Lecture Note Ser., Vol. 154, Cambridge Univ. Press, Cambridge, 1990, pp. 196–203. [21] LIARDET, P

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Complex variables approach to the short-axis-mode rotation of a rigid body

vector along the inertial z axis, the total angular momentum, and the projection of the angular momentum vector along the body axis of maximum inertia, respectively. The fact that the variables λ and μ are cyclic in Hamiltonian (1) immediately shows that the total angular momentum M as well as its projection along the z axis of the inertial frame Λ are integrals. Besides, because Λ is also ignorable in Eq. (1) , the node of the invariable plane remains fixed in the inertial x - y plane. Therefore, the free rigid body Hamiltonian in Andoyer variables is

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Poisson and symplectic reductions of 4–DOF isotropic oscillators. The van der Waals system as benchmark

},\overline{\mathscr{H}}_{\Xi,L_{1}}) \end{array}$ is a Lie-Poisson system, the corresponding dynamics is given by d K d t = 2 n ( β 2 − 4 )   S , d N d t = 2 [ 3 n ( 3 β 2 − 2 ) K + 2 ξ l ( 1 − β 2 ) ]   S , d S d t = n ( β 2 − 4 ) ( K 2 − ( ξ 2 + l 2 + n 2 ) ) K − ( 3 β 2 − 2 ) [ 6 n K N + 4 ξ l ( β 2 − 1 ) N + 2 l n 2 ξ ] . $$\begin{array}{} \displaystyle \begin{array}{*{20}{c}} {\frac{{dK}}{{dt}}} \hfill & = \hfill & {2n({\beta ^2} - 4){\kern 1pt} S,} \hfill \\ {\frac{{dN}}{{dt}}} \hfill & = \hfill & {2[3n(3{\beta ^2} - 2)K + 2\xi l(1 - {\beta ^2

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Degree-based indices computation for special chemical molecular structures using edge dividing method

1 8 16 10.1016/j.dam.2009.03.004 [41] J. Chen, J. Liu, Q. Li. (2013), The atom-bond connectivity index of catacondensed polyomino graphs, Discrete Dynamics in Nature and Society, vol. 2013, Article ID 598517, 7 pages. 10.1155/2013/598517 Chen J. Liu J. Li Q. 2013 The atom-bond connectivity index of catacondensed polyomino graphs Discrete Dynamics in Nature and Society 2013 Article ID 598517 7 doi 10.1155/2013/598517 [42] M. Eliasi, A. Iranmanesh. (2011), On ordinary generalized geometric-arithmetic index, Applied Mathematics Letters, 24, 582-587. 10.1016/j

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