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Predicting Rare Events via Large Deviations Theory: Rogue Waves and - - PowerPoint PPT Presentation

WCPM/CSC Seminar University of Warwick 30 Apr, 2018 Predicting Rare Events via Large Deviations Theory: Rogue Waves and Motile Bacteria Tobias Grafke, M. Cates, G. Dematteis, E. Vanden-Eijnden Rare events matter Rare events are important if


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WCPM/CSC Seminar

University of Warwick 30 Apr, 2018

Predicting Rare Events via Large Deviations Theory: Rogue Waves and Motile Bacteria

Tobias Grafke, M. Cates, G. Dematteis, E. Vanden-Eijnden

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SLIDE 2

Rare events matter Rare events are important if they are extreme Or separation of scales makes them common after all underlying dynamics might be very complex, and analytical solutions are not available in most cases: Turbulence, Climate, chemical- or biological systems Direct numerical simulations (sampling) is infeasible because events are very rare Rare events are often predictable: Requires computational approaches based on LDT

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 3

Large Deviation Theory The way rare events occur is often predictable — it is dominated by the least unlikely scenario — which is the essence of LDT Calculation of the least unlikely scenario (maximum likelihood pathway, MLP) reduces to a deterministic optimization problem

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Large Deviation Theory The way rare events occur is often predictable — it is dominated by the least unlikely scenario — which is the essence of LDT Calculation of the least unlikely scenario (maximum likelihood pathway, MLP) reduces to a deterministic optimization problem Simple example: gradient systems (navigating a potential landscape), transitions between local energy minima happen through minimum energy paths (mountain pass transition)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Large Deviation Theory The way rare events occur is often predictable — it is dominated by the least unlikely scenario — which is the essence of LDT Calculation of the least unlikely scenario (maximum likelihood pathway, MLP) reduces to a deterministic optimization problem Simple example: gradient systems (navigating a potential landscape), transitions between local energy minima happen through minimum energy paths (mountain pass transition)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 6

Large Deviation Theory The way rare events occur is often predictable — it is dominated by the least unlikely scenario — which is the essence of LDT Calculation of the least unlikely scenario (maximum likelihood pathway, MLP) reduces to a deterministic optimization problem Simple example: gradient systems (navigating a potential landscape), transitions between local energy minima happen through minimum energy paths (mountain pass transition)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 7

Large Deviation Theory The way rare events occur is often predictable — it is dominated by the least unlikely scenario — which is the essence of LDT Calculation of the least unlikely scenario (maximum likelihood pathway, MLP) reduces to a deterministic optimization problem Simple example: gradient systems (navigating a potential landscape), transitions between local energy minima happen through minimum energy paths (mountain pass transition)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 8

Large deviation theory for stochastic processes

A family of stochastic processes {Xε

t }t∈[0,T ] with smallness-parameter ε

(e.g. ε = 1/N, or ε = kBT, etc) fulfils large deviation principle: The probability that {Xε(t)}t∈[0,T ] is close to a path {φ(t)}t∈[0,T ] is Pε

  • sup

0≤t≤T

|Xε(t) − φ(t)| < δ

  • ≍ exp
  • −ε−1IT (φ)
  • for ε → 0

where IT (φ) is the rate function.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 9

Large deviation theory for stochastic processes

A family of stochastic processes {Xε

t }t∈[0,T ] with smallness-parameter ε

(e.g. ε = 1/N, or ε = kBT, etc) fulfils large deviation principle: The probability that {Xε(t)}t∈[0,T ] is close to a path {φ(t)}t∈[0,T ] is Pε

  • sup

0≤t≤T

|Xε(t) − φ(t)| < δ

  • ≍ exp
  • −ε−1IT (φ)
  • for ε → 0

where IT (φ) is the rate function. The probability of hitting set Az = {x|F(x) = z} is reduced to a minimisation problem Pε {Xε(T) ∈ Az|Xε(0) = x} ≍ exp

  • −ε−1

inf

φ:φ(0)=x,F (φ(T ))=z IT (φ)

  • Tobias Grafke

Predicting Rare Events via Large Deviations Theory

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SLIDE 10

Large deviation theory for stochastic processes

A family of stochastic processes {Xε

t }t∈[0,T ] with smallness-parameter ε

(e.g. ε = 1/N, or ε = kBT, etc) fulfils large deviation principle: The probability that {Xε(t)}t∈[0,T ] is close to a path {φ(t)}t∈[0,T ] is Pε

  • sup

0≤t≤T

|Xε(t) − φ(t)| < δ

  • ≍ exp
  • −ε−1IT (φ)
  • for ε → 0

where IT (φ) is the rate function. The probability of hitting set Az = {x|F(x) = z} is reduced to a minimisation problem Pε {Xε(T) ∈ Az|Xε(0) = x} ≍ exp

  • −ε−1

inf

φ:φ(0)=x,F (φ(T ))=z IT (φ)

  • Here, ≍ is log-asymptotic equivalence, i.e.

lim

ǫ→0 ε log Pε = − inf φ∈C IT (φ) with e.g. C =

  • {x}t∈[0,T ]|x(0) = x, F(x(T)) = z
  • Tobias Grafke

Predicting Rare Events via Large Deviations Theory

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SLIDE 11

Freidlin-Wentzell theory

In particular consider SDE (diffusion) for Xε

t ∈ Rn,

dXε

t = b(Xε t ) dt + √εσdWt ,

with “drift” b : Rn → Rn and “noise” with covariance χ = σσT , we have IT (φ) = 1

2

T | ˙ φ − b(φ)|2

χ dt =

T L(φ, ˙ φ) dt , for Lagrangian L(φ, ˙ φ) (follows by contraction from Schilder’s theorem). We are interested in φ∗ = argmin

φ∈C

T L(φ, ˙ φ) dt which is the maximum likelyhood pathway (MLP).

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Physicists approach: Path integral formalism

Consider ˙ x = b(x) + η with white noise η with covariance ηi(t)ηj(t′) = ǫχijδ(t − t′)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Physicists approach: Path integral formalism

Consider ˙ x = b(x) + η with white noise η with covariance ηi(t)ηj(t′) = ǫχijδ(t − t′) then P({η}) ∼

  • D[η] e− 1

  • ηχ−1η dt

but x = x[η], with η = ˙ x − b(x), so that (ignoring Jacobian) P({x}) ∼

  • D[x] e− 1

  • | ˙

x−b(x)|2

χ dt ∼

  • D[x] e− 1

ε IT (x)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 14

Physicists approach: Path integral formalism

Consider ˙ x = b(x) + η with white noise η with covariance ηi(t)ηj(t′) = ǫχijδ(t − t′) then P({η}) ∼

  • D[η] e− 1

  • ηχ−1η dt

but x = x[η], with η = ˙ x − b(x), so that (ignoring Jacobian) P({x}) ∼

  • D[x] e− 1

  • | ˙

x−b(x)|2

χ dt ∼

  • D[x] e− 1

ε IT (x)

Approximate path integral for ε → 0 via saddle point approximation, δI δφ∗ = 0, (Instanton, semi-classical trajectory)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 15

Physicists approach: Path integral formalism

Consider ˙ x = b(x) + η with white noise η with covariance ηi(t)ηj(t′) = ǫχijδ(t − t′) then P({η}) ∼

  • D[η] e− 1

  • ηχ−1η dt

but x = x[η], with η = ˙ x − b(x), so that (ignoring Jacobian) P({x}) ∼

  • D[x] e− 1

  • | ˙

x−b(x)|2

χ dt ∼

  • D[x] e− 1

ε IT (x)

Approximate path integral for ε → 0 via saddle point approximation, δI δφ∗ = 0, (Instanton, semi-classical trajectory) Rate function ↔ Action, MLP ↔ Instanton, LDP ↔ Hamiltonian principle

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Maximum likelyhood pathway and rare events

Main problem Find the maximum likelyhood pathway (MLP) φ∗ realizing an event, i.e. such that IT (φ∗) = inf

φ∈C IT (φ)

where C is the set of trajectories that fulfil our constraints.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 17

Maximum likelyhood pathway and rare events

Main problem Find the maximum likelyhood pathway (MLP) φ∗ realizing an event, i.e. such that IT (φ∗) = inf

φ∈C IT (φ)

where C is the set of trajectories that fulfil our constraints. Knowledge of the optimal trajectory gives us

  • 1. Probability of event, P ∼ exp
  • −ǫ−1IT (φ∗)
  • 2. Most likely occurence, φ∗ itself (allows for prediction, exploring

causes, etc.)

  • 3. Most effective way to force event (optimal control),
  • ptimal fluctuation

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Example: Ornstein-Uhlenbeck

Ornstein-Uhlenbeck process du = b(u) dt+dW , b(u) = −γu , γ > 0 . Consider extreme events with u(T) = z (so F(u) = u(T)). The instanton is u∗(t) = zeγ(t−T ) 1 − e−2γt 1 − e−2γT

  • ,
  • btained from constrained
  • ptimization

inf

{ut}∈Uz IT (z) =

inf

{ut}∈Uz 1 2

T | ˙ u+γu|2 dt

  • ver the set

Uz =

  • {ut}
  • F(uT ) = z
  • −10

−8 −6 −4 −2 t −1.0 −0.5 0.0 0.5 1.0 1.5 2.0 u(t) zeγ(t−T )

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Example: Ornstein-Uhlenbeck

Ornstein-Uhlenbeck process du = b(u) dt+dW , b(u) = −γu , γ > 0 . Consider extreme events with u(T) = z (so F(u) = u(T)). The instanton is u∗(t) = zeγ(t−T ) 1 − e−2γt 1 − e−2γT

  • ,
  • btained from constrained
  • ptimization

inf

{ut}∈Uz IT (z) =

inf

{ut}∈Uz 1 2

T | ˙ u+γu|2 dt

  • ver the set

Uz =

  • {ut}
  • F(uT ) = z
  • −10

−8 −6 −4 −2 t −1.0 −0.5 0.0 0.5 1.0 1.5 2.0 u(t) zeγ(t−T ) −10 −8 −6 −4 −2 t −1.0 −0.5 0.0 0.5 1.0 1.5 2.0 u(t)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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Example: Ornstein-Uhlenbeck

Ornstein-Uhlenbeck process du = b(u) dt+dW , b(u) = −γu , γ > 0 . Consider extreme events with u(T) = z (so F(u) = u(T)). The instanton is u∗(t) = zeγ(t−T ) 1 − e−2γt 1 − e−2γT

  • ,
  • btained from constrained
  • ptimization

inf

{ut}∈Uz IT (z) =

inf

{ut}∈Uz 1 2

T | ˙ u+γu|2 dt

  • ver the set

Uz =

  • {ut}
  • F(uT ) = z
  • −10

−8 −6 −4 −2 t −1.0 −0.5 0.0 0.5 1.0 1.5 2.0 u(t) zeγ(t−T ) average −10 −8 −6 −4 −2 t −1.0 −0.5 0.0 0.5 1.0 1.5 2.0 u(t)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 21

Reversible systems and gradient flows

Special case: Systems in detailed balance. For example, dXǫ

t = −∇U(Xǫ t ) dt +

√ 2ǫ dWt Then IT (φ) = 1

4

T | ˙ φ + ∇U|2 dt is minimized either by ˙ φ = −∇U (“sliding” down-hill) or IT (φ) = 1

4

T | ˙ φ + ∇U|2 dt = 1

4

T | ˙ φ − ∇U|2 dt + T ∇U · ˙ φ dt = U(φend) − U(φstart) if we choose ˙ φ = ∇U which is the time-reversed down-hill path. Easy algorithms exist∗.

∗Weinan E, Weiqing Ren, and Eric Vanden-Eijnden. “String method for the study of rare events”. In: Physical Review B

66.5 (Aug. 2002), p. 052301. doi: 10.1103/PhysRevB.66.052301.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 22

Example: Pendulum

Consider dampled pendulum dx = v dt + σ dWx, dv = − sin(x) dt − γv dt + σ dWv

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 23

Example: Pendulum

Consider dampled pendulum dx = v dt + σ dWx, dv = − sin(x) dt − γv dt + σ dWv

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 24

Example: Pendulum

Consider dampled pendulum dx = v dt + σ dWx, dv = − sin(x) dt − γv dt + σ dWv

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 25

Example: Pendulum

Consider dampled pendulum dx = v dt + σ dWx, dv = − sin(x) dt − γv dt + σ dWv

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 26

Hamiltonian formalism

Main problem Find the maximum likelyhood pathway (MLP) φ∗ realizing an event, i.e. such that IT (φ∗) = inf

φ∈C IT (φ)

where C is the set of trajectories that fulfil our constraints. Obtained through direct numerical minimisation,

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 27

Hamiltonian formalism

Main problem Find the maximum likelyhood pathway (MLP) φ∗ realizing an event, i.e. such that IT (φ∗) = inf

φ∈C IT (φ)

where C is the set of trajectories that fulfil our constraints. Obtained through direct numerical minimisation,

  • r through Hamiltionan

H(x, p) = sup

y

  • yp − L(x, y)

FW = b(x)p + 1

2pχp

so that (φ∗, θ∗) fulfil equations of motion    ˙ φ = ∇θH(φ, θ)

FW

= ⇒ ˙ φ = b(φ) + χθ ˙ θ = −∇φH(φ, θ)

FW

= ⇒ ˙ θ = −∇b(φ)T θ

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 28

Finding the minimizer

Algorithm†,‡: ˙ φ = b(φ) + χθ ˙ θ = −∇b(φ)T θ

φ θ t = 0 t = T

Advantages: Fits with the boundary conditions Simple time-integration scheme applicable (Runge-Kutta) No higher derivatives of H(φ, θ) This is essentially computing the gradient via the adjoint formalism

†A. I. Chernykh and M. G. Stepanov. “Large negative velocity gradients in Burgers turbulence”. In: Physical Review E

64.2 (July 2001), p. 026306. doi: 10.1103/PhysRevE.64.026306.

‡T. Grafke, R. Grauer, T. Sch ¨

afer, and E. Vanden-Eijnden. “Arclength Parametrized Hamilton’s Equations for the Calculation of Instantons”. In: Multiscale Modeling & Simulation 12.2 (Jan. 2014), pp. 566–580. issn: 1540-3459. doi: 10.1137/130939158.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 29

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 30

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 31

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 32

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

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SLIDE 33

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-34
SLIDE 34

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-35
SLIDE 35

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-36
SLIDE 36

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-37
SLIDE 37

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-38
SLIDE 38

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-39
SLIDE 39

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-40
SLIDE 40

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-41
SLIDE 41

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-42
SLIDE 42

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-43
SLIDE 43

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-44
SLIDE 44

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-45
SLIDE 45

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-46
SLIDE 46

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-47
SLIDE 47

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-48
SLIDE 48

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-49
SLIDE 49

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt)

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-50
SLIDE 50

Finding the minimizer

Algorithm§,¶:

φ θ t = 0 t = T

Problem for PDEs: Memory, e.g. 2D 2

  • (φ,θ)

× 1024 × 1024

  • space

× 104

  • time

≈ 1010 For θ: Store only χθ instead of θ, 10242 → 642 For φ: Recursive solution in φ, O(Nt) → O(log Nt) This is known as “checkpointing” in PDE optimization Additionally, bi-orthogonal wavelets to store fields

§Antonio Celani, Massimo Cencini, and Alain Noullez. “Going forth and back in time: a fast and parsimonious

algorithm for mixed initial/final-value problems”. In: Physica D: Nonlinear Phenomena 195.3 (2004), pp. 283–291.

¶Tobias Grafke, Rainer Grauer, and Stephan Schindel. “Efficient Computation of Instantons for Multi-Dimensional

Turbulent Flows with Large Scale Forcing”. In: Communications in Computational Physics 18.03 (Sept. 2015),

  • pp. 577–592. issn: 1991-7120. doi: 10.4208/cicp.031214.200415a.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-51
SLIDE 51

Finding the minimizer 128 256 512 1024 2048 4096 8192

Resolution

100 101 102 103

Memory Usage (in MB)

no optimization χθ recursive χθ & recursive

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-52
SLIDE 52

Application: Extreme gradients in Burgers equation

Evolution of Burgers shocks: ut + uux − νuxx = η with ηη′ = δ(t − t′)χ(x − x′) Compute P {ux(0, 0) > z|u(x, −T) = 0} Question: What is the most likely evolution from u(x)=0 at t=−∞, such that at the end (i.e. t = 0) we have a high gradient in the origin ux(x=0, t=0)=z (shock)?

Grafke, Grauer, Sch ¨ afer, and Vanden-Eijnden 2015

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-53
SLIDE 53

Application: Extreme gradients in Burgers equation

Evolution of Burgers shocks: ut + uux − νuxx = η with ηη′ = δ(t − t′)χ(x − x′) Compute P {ux(0, 0) > z|u(x, −T) = 0} Question: What is the most likely evolution from u(x)=0 at t=−∞, such that at the end (i.e. t = 0) we have a high gradient in the origin ux(x=0, t=0)=z (shock)?

Grafke, Grauer, Sch ¨ afer, and Vanden-Eijnden 2015

−300 −200 −100 a.u. −10−8−6−4−2 0 2 4 z −1.5 −1.0 −0.5 0.0 0.5 1.0 high Re med Re low Re Large deviations

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-54
SLIDE 54

Application: Extreme gradients in Burgers turbulence

¶Grafke, Grauer, and Sch ¨

afer 2013

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-55
SLIDE 55

Application: Extreme gradients in Burgers turbulence

H(u, θ) = θ · (u · ∇u − ν∇2u) + 1

2θχ ⋆ θ

  • dx

−20−15−10 −5 5 10 15 20 −6 −5 −4 −3 −2 −1 MLP −20−15−10 −5 5 10 15 20 −6 −5 −4 −3 −2 −1 Average event

¶Grafke, Grauer, and Sch ¨

afer 2013

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-56
SLIDE 56

Application: Active matter phase separation

Bacteria show complex collective behavior have active propulsion, i.e. a free-swimming (planktonic) stage are able to sense their environment through quorum sensing stick to surfaces in biofilms

  • E. Coli: active propulsion & biofilms

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-57
SLIDE 57

Application: Active matter phase separation

Bacteria show complex collective behavior have active propulsion, i.e. a free-swimming (planktonic) stage are able to sense their environment through quorum sensing stick to surfaces in biofilms Model bacteria as N agents with active Brownian motion, i.e. velocity vector diffuses on a sphere, density dependend diffusion constant, and birth/death

  • E. Coli: active propulsion & biofilms

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-58
SLIDE 58

Application: Active matter phase separation

Bacteria show complex collective behavior have active propulsion, i.e. a free-swimming (planktonic) stage are able to sense their environment through quorum sensing stick to surfaces in biofilms Model bacteria as N agents with active Brownian motion, i.e. velocity vector diffuses on a sphere, density dependend diffusion constant, and birth/death Then take LDT for N → ∞

  • E. Coli: active propulsion & biofilms

H(ρ, θ) = θ∂x(De(ρ)∂xρ − ρD(ρ)∂x(δ2∂2

xρ + θ)) + αρ(eθ − 1) + αρ2/ρ0(e−θ − 1)

  • dx

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-59
SLIDE 59

Application: Active matter phase separation

Complex collective behaviour for simple active agents: Propulsion and Reproduction When ρ0 < ρS, planktonic phase is robust. When ρS < ρ0 < ρc, particles

  • scillate between biofilm and

planktonic phase When ρc < ρ0, biofilms are

  • metastable. They rarely disperse

and reform by dying out Full phase diagram depends on carrying capacity ρ0 and domain size δ−1.

2 4 6 8 10 ρ0 5 10 15 20 25 30 35 δ−1 homogeneous quasi- periodic metastable

ρc ρS ¶Tobias Grafke, Michael E. Cates, and Eric Vanden-Eijnden. “Spatiotemporal Self-Organization of Fluctuating Bacterial

Colonies”. In: Physical Review Letters 119.18 (Nov. 2017), p. 188003. doi: 10.1103/PhysRevLett.119.188003

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-60
SLIDE 60

Application: Extreme ocean surface waves

Problem of Rogue waves: Creation mechanism not understood Probability unknown (but > Gaussian) Measurements difficult

(you might not be able to tell the tale)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-61
SLIDE 61

Application: Extreme ocean surface waves

Problem of Rogue waves: Creation mechanism not understood Probability unknown (but > Gaussian) Measurements difficult

(you might not be able to tell the tale)

Strategy: Random data from observation as input

JONSWAP spectrum

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-62
SLIDE 62

Application: Extreme ocean surface waves

Problem of Rogue waves: Creation mechanism not understood Probability unknown (but > Gaussian) Measurements difficult

(you might not be able to tell the tale)

Strategy: Random data from observation as input Accurate dynamical system to extrapolate output (MNLS)

JONSWAP spectrum

∂tu + 1

2∂xu + i 8∂2 xu − 1 16∂3 xu + i 2|u|2u + 3 2|u|2∂xu + 1 4u2∂xu∗ − i 2|∂x||u|2 = 0

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-63
SLIDE 63

Application: Extreme ocean surface waves

Problem of Rogue waves: Creation mechanism not understood Probability unknown (but > Gaussian) Measurements difficult

(you might not be able to tell the tale)

Strategy: Random data from observation as input Accurate dynamical system to extrapolate output (MNLS) Use LDT to obtain tails of height distribution

JONSWAP spectrum

∂tu + 1

2∂xu + i 8∂2 xu − 1 16∂3 xu + i 2|u|2u + 3 2|u|2∂xu + 1 4u2∂xu∗ − i 2|∂x||u|2 = 0

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-64
SLIDE 64

Application: Extreme ocean surface waves

rough sea (Hs = 3.3m, BFI = 0.34) high sea (Hs = 8.2m, BFI = 0.85)

2 4 6 8 10 12 14 16 H/m 100 10−2 10−4 10−6 10−8

rogue wave regime 0 min 5 min 10 min 15 min 20 min

5 10 15 20 25 30 H/m 100 10−2 10−4 10−6 10−8

rogue wave regime 0 min 1 min 2 min 3 min 5 min

Probability disctribution of spatial maximum of surface height

Monte-Carlo simulation (dots)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-65
SLIDE 65

Application: Extreme ocean surface waves

rough sea (Hs = 3.3m, BFI = 0.34) high sea (Hs = 8.2m, BFI = 0.85)

2 4 6 8 10 12 14 16 H/m 100 10−2 10−4 10−6 10−8

rogue wave regime 0 min 5 min 10 min 15 min 20 min

5 10 15 20 25 30 H/m 100 10−2 10−4 10−6 10−8

rogue wave regime 0 min 1 min 2 min 3 min 5 min

Probability disctribution of spatial maximum of surface height

Comparison between Monte-Carlo simulation (dots) and Large deviation theory (lines)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-66
SLIDE 66

Application: Extreme ocean surface waves

−4 −2 2 4 η/m

H = 8.5 m Hs = 3.3 m

t = 20 min Monte Carlo LDT −4 −2 2 4 η/m

H = 5.5 m Hs = 3.3 m

t = 10 min −2000 −1500 −1000 −500 500 1000 1500 2000 x/m −4 −2 2 4 η/m

H = 4.3 m Hs = 3.3 m

t = 0 min

¶Giovanni Dematteis, Tobias Grafke, and Eric Vanden-Eijnden. “Rogue waves and large deviations in deep sea”. In:

Proceedings of the National Academy of Sciences 115.5 (Jan. 2018), pp. 855–860. issn: 0027-8424, 1091-6490. doi: 10.1073/pnas.1710670115

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-67
SLIDE 67

LDT as WKB approximation

Consider Markov jump process with generator L, s.t. ∂tf = L†f (forward Kolmogorov, Fokker-Planck, Master eqn) ∂tf = Lf (backward Kolmogorov) e.g. for diffusion above, L = b · ∇ + 1

2ε∇∇

For WKB approximation, f ∼ exp

  • ε−1S
  • , BKE becomes to leading order

∂tf = b · ∇S + 1

2(∇S)2

which is a Hamilton-Jacobi equation, ∂tf = H(x, ∇S), H(x, p) = b · p + 1

2p2

This is the LDT Hamiltonian from before(!), but works for all MJP for additive Gaussian SDE for L´ evy processes

  • ther cases, i.e. stochastic

averaging for multiplicative Gaussian SDE for jump process

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-68
SLIDE 68

Challenges: Infinite transition time and geometric rate function

We actually want the most probable event regardless of duration. Drop the restriction of a pre-defined transition time T: I(˜ φ) = inf

T ∈(0,∞) inf φ IT (φ)

Possibly attains minimum at T → ∞.

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-69
SLIDE 69

Challenges: Infinite transition time and geometric rate function

We actually want the most probable event regardless of duration. Drop the restriction of a pre-defined transition time T: I(˜ φ) = inf

T ∈(0,∞) inf φ IT (φ)

Possibly attains minimum at T → ∞. Since H(φ, θ) = h = cst, we have

  • L(φ, ˙

φ) dt =

  • sup

θ

  • ˙

φ, θ − H(φ, θ)

  • dt =

sup

θ:H(φ,θ)=h

  • ˙

φ, θ dt + hT Effectively: Reduce minimisation over all paths to finding geodesic of the associated (almost Finsler) metric.

¶Heymann, Vanden-Eijnden (2008),

Grafke, Sch ¨ afer, Vanden-Eijnden (2017)

Tobias Grafke Predicting Rare Events via Large Deviations Theory

slide-70
SLIDE 70

Summary

Main theme Obtain statistics of and structures for rare events by numerically computing large deviation minimisers for spatially extended systems Challenges: Analytic solutions not available Needs PDE constrained

  • ptimisation (on GPUs)

Simplification necessary through nature of problem Applications: Fluid dynamic Non-equilibrium stat. mech. Rogue waves

Tobias Grafke Predicting Rare Events via Large Deviations Theory