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Research Group “Computational Time Series Analysis Institute of Mathematics Freie Universität Berlin (FU) Numerics of Stochastic Processes II (14.11.2008) Illia Horenko DFG Research Center MATHEON „Mathematics in key technologies“

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Page 1: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Research Group “Computational TimeSeries Analysis “Institute of MathematicsFreie

Universität

Berlin (FU)

Numerics of Stochastic Processes II(14.11.2008)Illia Horenko

DFG Research Center MATHEON „Mathematics

in key

technologies“

Page 2: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Short Reminder

Stochastic Processes

Discrete State Space,Discrete Time:Markov Chain

Discrete State Space,Continuous Time:Markov Process

Continuous State Space,Discrete Time:Markov Process

Continuous State Space,Continuous Time:Stochastic Differential Equation

Last Time

Page 3: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Short Reminder: Markov Processes

Infenitisimal Generator:

Markov Process Dynamics:

This Equation is Deterministic: ODE!

1) Numerical Methods from ODEs like Runge-Kutta-Method become available for stochatic processes

2) Monte-Carlo-Sampling just at the end!

Concepts from the Theory of Dynamical Systems are Applicable

Page 4: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Short Reminder

Stochastic Processes

Discrete State Space,Discrete Time:Markov Chain

Discrete State Space,Continuous Time:Markov Process

Continuous State Space,Discrete Time:Markov Process

Continuous State Space,Continuous Time:Stochastic Differential Equation

Today

Page 5: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Markov Process in R

Realizations of the process:

Process:

Next-Step Probability:

Next-Step Distribution:

This Equation is Deterministic!

Page 6: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Markov Process in R

Realizations of the process:

Process:

Next-Step Probability:

Next-Step Distribution:

This Equation is Deterministic!

Page 7: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Infenitisimal Generator:

Markov Process Dynamics:

This Equation is Deterministic: PDE!

1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available for stochatic processes

2) Monte-Carlo-Sampling just at the end!

Concepts from the Theory of Dynamical Systems are Applicable

Markov Process in R

Page 8: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Short Trip in the World ofDynamical Systems

Page 9: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Essential Dynamics of many dynamical systems is defined by attractors.

Attractor stays invariant under the

flow operator

Separation of informative (attractor) and non-informative (rest)parts of the space leads to dimension reduction

Dynamical

systems

viewpoint

Figures from http:\\w

ww

.wikipedia.org

Page 10: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Problem: Euclidean distance

cannot be used as a measure

for the

relative neighbourghood of attractor elements.

How

to localize

the

attractor?

Attractors can have very complex, even fractal geometry

Strategy: the data have to be “embedded“

into Eucllidean space

Whitney embedding theorem (Whitney, 1936) : sufficiently

smooth connected -dimensional manifolds can be smoothly

embedded in -dimensional Euclidean space.

Page 11: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Takens‘ Embedding (Takens, 1981)

and is a smooth map.

Assume that has an attractor with dimension

. Let , be a “proper“

measurement process. Then

is a -dimensional embedding in Euclidean space

How

to construct

the

embedding?

Page 12: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Illustration of Takens‘

EmbeddingThe image of is unfolded in

Problems:-

how to “filter out“

the attractive subspace?

-

how to connect the changes in attractive subspace

with hiddenphase?

Strategy:

Let . Define a

new variable

. Let the attractor for

each of the hidden phases be contained in a distinct linear

manifold defined via

Page 13: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Topological

dimension

reduction

(H. 07): for a given time series we look for a

minimum of the reconstruction error

μ

T

Page 14: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Topological

dimension

reduction

(H. 07): for a given time series we look for a

minimum of the reconstruction error

μ

(X-μ)

TT (X-μ)T

Txt

t

t

Page 15: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Topological

dimension

reduction

(H. 07): for a given time series we look for a

minimum of the reconstruction error

μ

(X-μ)

TT (X-μ)T

Txt

t

t

Page 16: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Analysis of embedded

data

PCA + Takens‘ Embedding (Broomhead&King, 1986)

Let . Define a new variable

. Let the attractor

from Takens‘

Theorem be in a linear manifold defined via

. Then

Reconstruction from m

essential coordinates:

Page 17: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

PCA+Takens: data

compression/reconstruction

1.

2.

3.

4.

5.

Page 18: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

0

10

20

30

40

50

−20−10

010

2030

−40

−20

0

20

40

Lorenz-Oszillator with measurement noise

Example: Lorenz

Page 19: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

Example: Lorenz

Reconstructed trajectory(red, for m=2)

Page 20: Numerics of Stochastic Processes II (14.11.2008)page.mi.fu-berlin.de/horenko/download/NumerikIV/VL_5.pdf1) Numerical Methods from PDEs like Finite-Element-Methods (FEM) become available

1) Markov-Prozesse (I): Dynamische Systeme und Identifikation der metastabilen Mengen (Maren)

2) Markov-Prozesse (II): Generatorschätzung (??)

3) Large Deviations Theory (Olga)

4) Dimensionsreduktion in Datenanalyse: graphentheoretische Zugänge I (Paul)

5) Dimensionsreduktion in Datenanalyse: graphentheoretische Zugänge II(Ilja)

6) Prozesse mit Errinerung (I): opt. Steuerung, Kalman-Filter und ARMAX-Model (??)

7) Prozesse mit Errinerung (II): Change-Point analysis (Peter)

8) Varianz von Parameterschätzungen (Bootstrap-Algorithmus) (Beatrice)

9) Modelvergleich in Finanzsektor (Lars)

Themen