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MAX PLANCK INSTITUTE FOR DYNAMICS OF COMPLEX TECHNICAL SYSTEMS MAGDEBURG February 13, 2013 Balanced Truncation for Stochastic Differential Equations with Levy Noise Martin Redmann Computational Methods in Systems and Control Theory Max Planck Institute for Dynamics of Complex Technical Systems Magdeburg, Germany Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 1/25

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  • MAX PLANCK INSTITUTE

    FOR DYNAMICS OF COMPLEX

    TECHNICAL SYSTEMS

    MAGDEBURG

    February 13, 2013

    Balanced Truncation for StochasticDifferential Equations with Levy Noise

    Martin Redmann

    Computational Methods in Systems and Control TheoryMax Planck Institute for Dynamics of Complex Technical Systems

    Magdeburg, Germany

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 1/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Content

    1 Introduction

    2 Concept of Reachability

    3 Concept of Observability

    4 Balanced Truncation

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 2/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Content

    1 Introduction

    2 Concept of Reachability

    3 Concept of Observability

    4 Balanced Truncation

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 2/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Content

    1 Introduction

    2 Concept of Reachability

    3 Concept of Observability

    4 Balanced Truncation

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 2/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Content

    1 Introduction

    2 Concept of Reachability

    3 Concept of Observability

    4 Balanced Truncation

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 2/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Levy processes

    Properties of Levy processes

    Levy processes generalize Wiener processes.

    The trajectories may have jumps but at most countably many.

    The trajectories are right-continuous and have left limits.

    We will focus on square integrable Levy processes (M(t))t≥0 with zeromean, which means that

    E [M(t)] = 0 and E[M(t)2

    ]

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Levy processes

    Properties of Levy processes

    Levy processes generalize Wiener processes.

    The trajectories may have jumps but at most countably many.

    The trajectories are right-continuous and have left limits.

    We will focus on square integrable Levy processes (M(t))t≥0 with zeromean, which means that

    E [M(t)] = 0 and E[M(t)2

    ]

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Levy processes

    Properties of Levy processes

    Levy processes generalize Wiener processes.

    The trajectories may have jumps but at most countably many.

    The trajectories are right-continuous and have left limits.

    We will focus on square integrable Levy processes (M(t))t≥0 with zeromean, which means that

    E [M(t)] = 0 and E[M(t)2

    ]

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Levy processes

    Properties of Levy processes

    Levy processes generalize Wiener processes.

    The trajectories may have jumps but at most countably many.

    The trajectories are right-continuous and have left limits.

    We will focus on square integrable Levy processes (M(t))t≥0 with zeromean, which means that

    E [M(t)] = 0 and E[M(t)2

    ]

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Levy processes

    Properties of Levy processes

    Levy processes generalize Wiener processes.

    The trajectories may have jumps but at most countably many.

    The trajectories are right-continuous and have left limits.

    We will focus on square integrable Levy processes (M(t))t≥0 with zeromean, which means that

    E [M(t)] = 0 and E[M(t)2

    ]

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider the following equation for t ≥ 0:

    dX (t) = [AX (t) + Bu(t)] dt + ΨX (t−)dM(t), (1)Y(t) = CX (t),

    where X (0) = x0, A,Ψ ∈ Rn×n, B ∈ Rn×m, C ∈ Rp×n, M is areal-valued square integrable Levy process with zero mean and u is anadapted stochastic processes with

    ‖u‖2L2 := E∫ ∞

    0

    ‖u(t)‖22 dt

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider the following equation for t ≥ 0:

    dX (t) = [AX (t) + Bu(t)] dt + ΨX (t−)dM(t), (1)Y(t) = CX (t),

    where X (0) = x0, A,Ψ ∈ Rn×n, B ∈ Rn×m, C ∈ Rp×n, M is areal-valued square integrable Levy process with zero mean and u is anadapted stochastic processes with

    ‖u‖2L2 := E∫ ∞

    0

    ‖u(t)‖22 dt

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Fundamental Solution

    We introduce the stochastic processes (Φ(t, τ))t≥τ with values in Rn×n,which satify

    Φ(t, τ) = In +

    ∫ tτ

    AΦ(s, τ)ds +

    ∫ tτ

    ΨΦ(s−, τ)dM(s)

    for t ≥ τ ≥ 0. We write Φ(t, 0) = Φ(t).

    Proposition

    The solution of equation (1) is given by

    Φ(t)x0 +

    ∫ t0

    Φ(t, s)Bu(s)ds, t ≥ 0.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 5/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Fundamental Solution

    We introduce the stochastic processes (Φ(t, τ))t≥τ with values in Rn×n,which satify

    Φ(t, τ) = In +

    ∫ tτ

    AΦ(s, τ)ds +

    ∫ tτ

    ΨΦ(s−, τ)dM(s)

    for t ≥ τ ≥ 0. We write Φ(t, 0) = Φ(t).

    Proposition

    The solution of equation (1) is given by

    Φ(t)x0 +

    ∫ t0

    Φ(t, s)Bu(s)ds, t ≥ 0.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 5/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Concept of Reachability

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 6/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Reachability Gramian [Benner, Damm ’11]

    We call Pt :=∫ t

    0E[Φ(s)BBT ΦT (s)

    ]ds finite reachability Gramian at

    time t ≥ 0.The asymptotic stability in mean square also provides the existence of theinfinite reachability Gramian

    P :=

    ∫ ∞0

    E[Φ(s)BBT ΦT (s)

    ]ds.

    Proposition

    For all t ≥ 0 it holds

    im Pt = im P.

    One can show that

    0 = BBT + P AT + A P + Ψ P ΨT E[M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 7/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Reachability Gramian [Benner, Damm ’11]

    We call Pt :=∫ t

    0E[Φ(s)BBT ΦT (s)

    ]ds finite reachability Gramian at

    time t ≥ 0.The asymptotic stability in mean square also provides the existence of theinfinite reachability Gramian

    P :=

    ∫ ∞0

    E[Φ(s)BBT ΦT (s)

    ]ds.

    Proposition

    For all t ≥ 0 it holds

    im Pt = im P.

    One can show that

    0 = BBT + P AT + A P + Ψ P ΨT E[M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 7/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Reachability Gramian [Benner, Damm ’11]

    We call Pt :=∫ t

    0E[Φ(s)BBT ΦT (s)

    ]ds finite reachability Gramian at

    time t ≥ 0.The asymptotic stability in mean square also provides the existence of theinfinite reachability Gramian

    P :=

    ∫ ∞0

    E[Φ(s)BBT ΦT (s)

    ]ds.

    Proposition

    For all t ≥ 0 it holds

    im Pt = im P.

    One can show that

    0 = BBT + P AT + A P + Ψ P ΨT E[M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 7/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Reachability Gramian [Benner, Damm ’11]

    We call Pt :=∫ t

    0E[Φ(s)BBT ΦT (s)

    ]ds finite reachability Gramian at

    time t ≥ 0.The asymptotic stability in mean square also provides the existence of theinfinite reachability Gramian

    P :=

    ∫ ∞0

    E[Φ(s)BBT ΦT (s)

    ]ds.

    Proposition

    For all t ≥ 0 it holds

    im Pt = im P.

    One can show that

    0 = BBT + P AT + A P + Ψ P ΨT E[M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 7/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    By X (T , 0, u) we denote the solution of the inhomogeneous system (1)at time T with initial condition 0 for a given input u.

    Definition

    An avarage state x ∈ Rn is called reachable (from zero) if a time T > 0and a control function u ∈ L2T exist such that

    E [X (T , 0, u)] = x .

    Proposition

    An avarage state x ∈ Rn is reachable (from zero) if and only if x ∈ im P.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 8/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    By X (T , 0, u) we denote the solution of the inhomogeneous system (1)at time T with initial condition 0 for a given input u.

    Definition

    An avarage state x ∈ Rn is called reachable (from zero) if a time T > 0and a control function u ∈ L2T exist such that

    E [X (T , 0, u)] = x .

    Proposition

    An avarage state x ∈ Rn is reachable (from zero) if and only if x ∈ im P.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 8/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    By X (T , 0, u) we denote the solution of the inhomogeneous system (1)at time T with initial condition 0 for a given input u.

    Definition

    An avarage state x ∈ Rn is called reachable (from zero) if a time T > 0and a control function u ∈ L2T exist such that

    E [X (T , 0, u)] = x .

    Proposition

    An avarage state x ∈ Rn is reachable (from zero) if and only if x ∈ im P.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 8/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Proposition

    The control u with minimal energy to reach x ∈ im P at time T > 0 isgiven by

    u(t) = BT ΦT (T , t)P#T x , t ∈ [0,T ],

    with

    ‖u‖2L2T = xTP#T x .

    Thus, the minimal energy that is needed to steer the system to x is givenby

    infT>0

    xTP#T x = xTP#x .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 9/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Proposition

    The control u with minimal energy to reach x ∈ im P at time T > 0 isgiven by

    u(t) = BT ΦT (T , t)P#T x , t ∈ [0,T ],

    with

    ‖u‖2L2T = xTP#T x .

    Thus, the minimal energy that is needed to steer the system to x is givenby

    infT>0

    xTP#T x = xTP#x .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 9/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Concept of Observability

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 10/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Observability Gramian [Benner, Damm ’11]

    Due to the asymptotic stability in mean square the observability Gramian

    Q = E[∫ ∞

    0

    ΦT (s)CTCΦ(s)ds

    ]exists and it is the solution of

    AT Q + Q A + ΨTQΨ E[M(1)2

    ]+ CTC = 0.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 11/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider an uncontrolled system (1) (u ≡ 0).Hence, X (t) = Φ(t)x0 and

    Y(t) = CΦ(t)x0.

    The observation energy produced by x0 is

    ‖Y‖2L2 := E∫ ∞

    0

    YT (t)Y(t)dt = xT0 E∫ ∞

    0

    ΦT (t)CTCΦ(t)dt x0

    = xT0 Qx0.

    DefinitionAn inital condition x0 is unobservable if x0 ∈ ker Q.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 12/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider an uncontrolled system (1) (u ≡ 0).Hence, X (t) = Φ(t)x0 and

    Y(t) = CΦ(t)x0.

    The observation energy produced by x0 is

    ‖Y‖2L2 := E∫ ∞

    0

    YT (t)Y(t)dt = xT0 E∫ ∞

    0

    ΦT (t)CTCΦ(t)dt x0

    = xT0 Qx0.

    DefinitionAn inital condition x0 is unobservable if x0 ∈ ker Q.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 12/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider an uncontrolled system (1) (u ≡ 0).Hence, X (t) = Φ(t)x0 and

    Y(t) = CΦ(t)x0.

    The observation energy produced by x0 is

    ‖Y‖2L2 := E∫ ∞

    0

    YT (t)Y(t)dt = xT0 E∫ ∞

    0

    ΦT (t)CTCΦ(t)dt x0

    = xT0 Qx0.

    DefinitionAn inital condition x0 is unobservable if x0 ∈ ker Q.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 12/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Balanced Truncation

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 13/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We start with a system

    dX (t) = [AX (t) + Bu(t)] dt + ΨX (t−)dM(t), (2)Y(t) = CX (t), t ≥ 0,

    which is completely reachable and observable, which is equivalent to Pand Q are positive definite.

    We transfer the states with a regular matrix T and obtain a system with

    (Ã, B̃, Ψ̃, C̃ ) = (TAT−1,TB,TΨT−1,CT−1),

    which has the same output as system (2).

    The Gramians of the transformed system are given by

    P̃ = TPTT and Q̃ = T−TQT−1.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 14/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We start with a system

    dX (t) = [AX (t) + Bu(t)] dt + ΨX (t−)dM(t), (2)Y(t) = CX (t), t ≥ 0,

    which is completely reachable and observable, which is equivalent to Pand Q are positive definite.

    We transfer the states with a regular matrix T and obtain a system with

    (Ã, B̃, Ψ̃, C̃ ) = (TAT−1,TB,TΨT−1,CT−1),

    which has the same output as system (2).

    The Gramians of the transformed system are given by

    P̃ = TPTT and Q̃ = T−TQT−1.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 14/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We start with a system

    dX (t) = [AX (t) + Bu(t)] dt + ΨX (t−)dM(t), (2)Y(t) = CX (t), t ≥ 0,

    which is completely reachable and observable, which is equivalent to Pand Q are positive definite.

    We transfer the states with a regular matrix T and obtain a system with

    (Ã, B̃, Ψ̃, C̃ ) = (TAT−1,TB,TΨT−1,CT−1),

    which has the same output as system (2).

    The Gramians of the transformed system are given by

    P̃ = TPTT and Q̃ = T−TQT−1.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 14/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Balancing Transformation

    We want to choose T , such that the Gramians are equal, which meansthat P̃ = Q̃ = Σ = diag(σ1, . . . , σn).

    TheoremThe balancing transformation T and its inverse are given by

    T = Σ12 KTU−1,

    T−1 = UKΣ−12 ,

    where P = UUT and UTQU = KΣ2KT .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 15/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider the following partitions:

    T =

    [W T

    TT2

    ], T−1 =

    [V T1

    ]and X̂ =

    (X̃X1

    ),

    where W T ∈ Rr×n,V ∈ Rn×r and X̃ ∈ Rr .

    Hence,(dX̃ (t)dX1(t)

    )=

    [W TAV W TAT1TT2 AV T

    T2 AT1

    ](X̃ (t)X1(t)

    )dt +

    [W TBTT2 B

    ]u(t)dt

    +

    [W T ΨV W T ΨT1TT2 ΨV T

    T2 ΨT1

    ](X̃ (t−)X1(t−)

    )dM(t)

    and

    Y(t) =[CV CT1

    ]( X̃ (t)X1(t)

    ).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 16/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We consider the following partitions:

    T =

    [W T

    TT2

    ], T−1 =

    [V T1

    ]and X̂ =

    (X̃X1

    ),

    where W T ∈ Rr×n,V ∈ Rn×r and X̃ ∈ Rr .

    Hence,(dX̃ (t)dX1(t)

    )=

    [W TAV W TAT1TT2 AV T

    T2 AT1

    ](X̃ (t)X1(t)

    )dt +

    [W TBTT2 B

    ]u(t)dt

    +

    [W T ΨV W T ΨT1TT2 ΨV T

    T2 ΨT1

    ](X̃ (t−)X1(t−)

    )dM(t)

    and

    Y(t) =[CV CT1

    ]( X̃ (t)X1(t)

    ).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 16/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Selecting the first r rows and neglecting the X1 terms provide thefollowing reduced order model:

    dX̃ (t) = W TAV X̃ (t)dt + W TBu(t)dt + W T ΨV X̃ (t−)dM(t)Ỹ(t) = CV X̃ (t).

    Open Questions1 Is the reduced order model stable in general?

    deterministic case: The reduced order model is stable.

    2 What is the structure of the Gramians of the reduced model?deterministic case: PR = QR = diag(σ1, . . . , σr )

    3 What is the structure of the Hankel values of the reduced model?deterministic case: The Hankel values are σ1, . . . , σr .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 17/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Selecting the first r rows and neglecting the X1 terms provide thefollowing reduced order model:

    dX̃ (t) = W TAV X̃ (t)dt + W TBu(t)dt + W T ΨV X̃ (t−)dM(t)Ỹ(t) = CV X̃ (t).

    Open Questions1 Is the reduced order model stable in general?

    deterministic case: The reduced order model is stable.

    2 What is the structure of the Gramians of the reduced model?deterministic case: PR = QR = diag(σ1, . . . , σr )

    3 What is the structure of the Hankel values of the reduced model?deterministic case: The Hankel values are σ1, . . . , σr .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 17/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Selecting the first r rows and neglecting the X1 terms provide thefollowing reduced order model:

    dX̃ (t) = W TAV X̃ (t)dt + W TBu(t)dt + W T ΨV X̃ (t−)dM(t)Ỹ(t) = CV X̃ (t).

    Open Questions1 Is the reduced order model stable in general?

    deterministic case: The reduced order model is stable.

    2 What is the structure of the Gramians of the reduced model?deterministic case: PR = QR = diag(σ1, . . . , σr )

    3 What is the structure of the Hankel values of the reduced model?deterministic case: The Hankel values are σ1, . . . , σr .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 17/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Selecting the first r rows and neglecting the X1 terms provide thefollowing reduced order model:

    dX̃ (t) = W TAV X̃ (t)dt + W TBu(t)dt + W T ΨV X̃ (t−)dM(t)Ỹ(t) = CV X̃ (t).

    Open Questions1 Is the reduced order model stable in general?

    deterministic case: The reduced order model is stable.

    2 What is the structure of the Gramians of the reduced model?deterministic case: PR = QR = diag(σ1, . . . , σr )

    3 What is the structure of the Hankel values of the reduced model?deterministic case: The Hankel values are σ1, . . . , σr .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 17/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    The following matrices provide a balanced system:

    A =(−5.12 2.99 2.05

    1.25 −4.86 0.961.26 0.07 −9.52

    ),B =

    (−3.39 −1.19 −0.611.31 −4.60 −0.09−0.68 1.70 4.57

    ),

    Ψ =(−2.20 2.09 −0.57

    1.30 −0.67 −2.060.30 −0.57 −1.14

    ),C =

    (−2.77 1.31 1.62−3.94 −2.18 0.74−1.31 −2.49 1.74

    ).

    The Gramians are given by

    P = Q = Σ =(

    5.97 0 00 4.23 00 0 1.48

    ).

    The reduced order model has the following properties:

    PR =(

    5.46 −0.38−0.38 3.43

    ),QR = ( 5.88 0.060.06 4.16 ) ,HVR = (

    5.683.76 ) .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 18/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    The following matrices provide a balanced system:

    A =(−5.12 2.99 2.05

    1.25 −4.86 0.961.26 0.07 −9.52

    ),B =

    (−3.39 −1.19 −0.611.31 −4.60 −0.09−0.68 1.70 4.57

    ),

    Ψ =(−2.20 2.09 −0.57

    1.30 −0.67 −2.060.30 −0.57 −1.14

    ),C =

    (−2.77 1.31 1.62−3.94 −2.18 0.74−1.31 −2.49 1.74

    ).

    The Gramians are given by

    P = Q = Σ =(

    5.97 0 00 4.23 00 0 1.48

    ).

    The reduced order model has the following properties:

    PR =(

    5.46 −0.38−0.38 3.43

    ),QR = ( 5.88 0.060.06 4.16 ) ,HVR = (

    5.683.76 ) .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 18/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    The following matrices provide a balanced system:

    A =(−5.12 2.99 2.05

    1.25 −4.86 0.961.26 0.07 −9.52

    ),B =

    (−3.39 −1.19 −0.611.31 −4.60 −0.09−0.68 1.70 4.57

    ),

    Ψ =(−2.20 2.09 −0.57

    1.30 −0.67 −2.060.30 −0.57 −1.14

    ),C =

    (−2.77 1.31 1.62−3.94 −2.18 0.74−1.31 −2.49 1.74

    ).

    The Gramians are given by

    P = Q = Σ =(

    5.97 0 00 4.23 00 0 1.48

    ).

    The reduced order model has the following properties:

    PR =(

    5.46 −0.38−0.38 3.43

    ),QR = ( 5.88 0.060.06 4.16 ) ,HVR = (

    5.683.76 ) .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 18/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Error Bound

    We introduce the following partitions of a balanced realization:

    A =[

    A11 A12A21 A22

    ], Ψ =

    [Ψ11 Ψ12Ψ21 Ψ22

    ], B =

    [B1B2

    ]and C = [ C1 C2 ] .

    We write E = E∥∥Y(t)− Ỹ(t)∥∥

    2and obtain

    E = E∥∥∥∥C ∫ t

    0

    Φ(t, s)Bu(s)ds − C1∫ t

    0

    Φ̃(t, s)B1u(s)ds

    ∥∥∥∥2

    ≤ E∫ t

    0

    ∥∥∥(CΦ(t, s)B − C1Φ̃(t, s)B1) u(s)∥∥∥2ds

    ≤ E∫ t

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥F‖u(s)‖2 ds

    ≤(E∫ t

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥2Fds

    ) 12(E∫ t

    0

    ‖u(s)‖22 ds) 1

    2

    .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 19/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Error Bound

    We introduce the following partitions of a balanced realization:

    A =[

    A11 A12A21 A22

    ], Ψ =

    [Ψ11 Ψ12Ψ21 Ψ22

    ], B =

    [B1B2

    ]and C = [ C1 C2 ] .

    We write E = E∥∥Y(t)− Ỹ(t)∥∥

    2and obtain

    E = E∥∥∥∥C ∫ t

    0

    Φ(t, s)Bu(s)ds − C1∫ t

    0

    Φ̃(t, s)B1u(s)ds

    ∥∥∥∥2

    ≤ E∫ t

    0

    ∥∥∥(CΦ(t, s)B − C1Φ̃(t, s)B1) u(s)∥∥∥2ds

    ≤ E∫ t

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥F‖u(s)‖2 ds

    ≤(E∫ t

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥2Fds

    ) 12(E∫ t

    0

    ‖u(s)‖22 ds) 1

    2

    .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 19/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We have

    supt≥0

    E∥∥Y(t)− Ỹ(t)∥∥

    2

    ≤(E∫ ∞

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥2Fds

    ) 12

    ︸ ︷︷ ︸#

    ‖u‖L2 .

    It holds

    # =(tr(CΣCT

    )+ tr

    (C1PRC

    T1

    )− 2 tr

    (CPMC

    T1

    )) 12 ,

    where

    0 = BBT1 + PMAT11 + APM + ΨPM Ψ

    T11 E

    [M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 20/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We have

    supt≥0

    E∥∥Y(t)− Ỹ(t)∥∥

    2

    ≤(E∫ ∞

    0

    ∥∥∥CΦ(t, s)B − C1Φ̃(t, s)B1∥∥∥2Fds

    ) 12

    ︸ ︷︷ ︸#

    ‖u‖L2 .

    It holds

    # =(tr(CΣCT

    )+ tr

    (C1PRC

    T1

    )− 2 tr

    (CPMC

    T1

    )) 12 ,

    where

    0 = BBT1 + PMAT11 + APM + ΨPM Ψ

    T11 E

    [M(1)2

    ].

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 20/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Special Case

    We assume

    Ψ =

    [Ψ11 0

    0 Ψ22

    ].

    We additionally need the partitions

    Σ =

    [Σ1

    Σ2

    ]and PM =

    [PM,1PM,2

    ].

    Then, PR = QR = Σ1 and

    #2 = tr((CT2 C2 + 2PM,2AT21)Σ2).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 21/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    How to check stability of the reduced order model?

    Theorem see [Damm ’04]

    Let Y be an arbitrary symmetric and negative definite matrix. Then, thereduced order model is asymptotically mean square stable, if and only ifthe solution X of

    AT11X + XA11 + ΨT11XΨ11 E

    [M(1)2

    ]= Y

    is unique, symmetric and positive definite.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 22/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    We consider a company, which produces n goods.Xi represents the asset of the company corresponding to good i .

    We assume that the vector of all assets satisfies

    dX (t) = [u(t)− diag(λ1, . . . , λn)X (t)] dt + X (t−)dM(t)X (0) = x0,

    where λi is the depreciation rate of Xi and u is the vector of investments.

    We observe that the system is asymptotically mean square stable if andonly if λi > 0.5 E

    [M(1)2

    ]for all i = 1, . . . , n.

    The output equation we consider is given by

    Y (t) = (1, . . . , 1)X (t).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 23/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    We consider a company, which produces n goods.Xi represents the asset of the company corresponding to good i .

    We assume that the vector of all assets satisfies

    dX (t) = [u(t)− diag(λ1, . . . , λn)X (t)] dt + X (t−)dM(t)X (0) = x0,

    where λi is the depreciation rate of Xi and u is the vector of investments.

    We observe that the system is asymptotically mean square stable if andonly if λi > 0.5 E

    [M(1)2

    ]for all i = 1, . . . , n.

    The output equation we consider is given by

    Y (t) = (1, . . . , 1)X (t).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 23/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    We consider a company, which produces n goods.Xi represents the asset of the company corresponding to good i .

    We assume that the vector of all assets satisfies

    dX (t) = [u(t)− diag(λ1, . . . , λn)X (t)] dt + X (t−)dM(t)X (0) = x0,

    where λi is the depreciation rate of Xi and u is the vector of investments.

    We observe that the system is asymptotically mean square stable if andonly if λi > 0.5 E

    [M(1)2

    ]for all i = 1, . . . , n.

    The output equation we consider is given by

    Y (t) = (1, . . . , 1)X (t).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 23/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Example

    We consider a company, which produces n goods.Xi represents the asset of the company corresponding to good i .

    We assume that the vector of all assets satisfies

    dX (t) = [u(t)− diag(λ1, . . . , λn)X (t)] dt + X (t−)dM(t)X (0) = x0,

    where λi is the depreciation rate of Xi and u is the vector of investments.

    We observe that the system is asymptotically mean square stable if andonly if λi > 0.5 E

    [M(1)2

    ]for all i = 1, . . . , n.

    The output equation we consider is given by

    Y (t) = (1, . . . , 1)X (t).

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 23/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    We assume that n = 80, E[M(1)2

    ]= 1 and λi ∈ (0.5, 1.5]:

    Dimension of reduced order model #

    40 7.2277 · 10−620 7.2237 · 10−610 0.00265 0.35172 4.5929

    .

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 24/25

  • Introduction Concept of Reachability Concept of Observability Balanced Truncation

    Thank you for your attention!

    ReferencesAntoulas ’05: Approximation of large-scale dynamical systems,Advances in Design and Control 6. Philadelphia, PA: Society for Industrialand Applied Mathematics (SIAM).

    Applebaum ’09: Lèvy Processes and Stochastic Calculus, CambridgeStudies in Advanced Mathematics 116. Cambridge: Cambridge UniversityPress.

    Benner, Damm ’11: Lyapunov equations, energy functionals, and modelorder reduction of bilinear and stochastic systems, SIAM J. ControlOptim., 49(2):686-711, 2011.

    Damm ’04: Rational Matrix Equations in Stochastic Control, LectureNotes in Control and Information Sciences 297. Berlin: Springer.

    Max Planck Institute Magdeburg M. Redmann, Balanced Truncation for Stochastic Differential Equations with Levy Noise 25/25

    IntroductionConcept of ReachabilityConcept of ObservabilityBalanced Truncation