Non-Linear Time Series 2nd part.ppt


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Non-Linear Time Series … 2nd part
Léonard Studer
IPHE-UNIL
leonard.******@
11/10/2017
1
Refresh on chaotic dynamical systems theory 1/2
Necessary cond to have dyn chaos:
Either system of differential equations with 3 or more degrees of freedom
Or invertible discrete time maps with 2 or more dof
Logistic map is a noninvertible map with 1 dof that can show chaos
11/10/2017
2
Léonard Studer, IPHE-UNIL
Refresh from chaotic dynamical systems theory 2/2
BUT chaos has structure in phase space
Chaos is irregular in time and slightly predictable
11/10/2017
3
Léonard Studer, IPHE-UNIL
Main steps in nonlinear time series proc’g 2/2
Simple nonlinear noise reduction

Control

A lot of new applications are actively studied in academic and private labs (see ref Proceedings of the IEEE)
Synchronization of chaotic systems,
chaos-based techniques for spread-spectrum sequences generation,
modulation based on chaotic signal,
Cryptographic coding with chaos etc
Not detailed presented today,
11/10/2017
4
Léonard Studer, IPHE-UNIL
Simple nonlinear noise reduction
n0-2
n0-1
n0
n0+1
Select trajectories that stay close for a few time steps to the segment to be cleaned. Below only trajectory X is OK
The filtered-cleaned-new value x’n0 is the average value of scalars sj that are in the ball neighborhood of the xn0 !
X
11/10/2017
5
Léonard Studer, IPHE-UNIL
Example of simple noise reduction
Time series is air flow through the nose of a human as an indicator of breath activity (example from TISEAN tutorial, see ref)
11/10/2017
6
Léonard Studer, IPHE-UNIL
Advanced methods in nonlinear noise reduction
Refinements of the 2nd step
local projective noise reduction
ANN etc
nonlinear noise reduction in a data stream
Here, only past sj values are known…
But it can be done !
See T. Schreiber and M. Richter, Nonlinear projective filtering in a data stream, in Int. J. Bifurcat. Chaos (1999).
11/10/2017
7
Léonard Studer, IPHE-UNIL
Unstable Pe

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  • 时间2011-08-29