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Monotone Dynamical Systems: A Quick Tour Hal Smith A R I Z O N A S - - PowerPoint PPT Presentation

Monotone Dynamical Systems: A Quick Tour Hal Smith A R I Z O N A S T A T E U N I V E R S I T Y H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 1 / 16 Monotone Dynamical System State space: metric space ( X , d ) with a


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Monotone Dynamical Systems: A Quick Tour

Hal Smith

A R I Z O N A S T A T E U N I V E R S I T Y

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 1 / 16

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Monotone Dynamical System

1

State space: metric space (X, d) with a closed* partial order relation ≤.

*(xn ≤ yn ∧ xn → x ∧ yn → y ⇒ x ≤ y) 2

Dynamics: discrete-time (T = Z+) or continuous-time (T = R+) semiflow Φ : T × X → X. Notation Φt(x) = Φ(t, x):

Φ continuous. Φ0 = idX Φt ◦ Φs = Φt+s, t, s ∈ T

3

Order-Preserving: x ≤ y ⇒ Φt(x) ≤ Φt(y), t ∈ T, x, y ∈ X.

Trivial Examples: X = R, usual order ≤, x′ = f(x), Φt(x0) = x(t, x0). X = BC(R, R), usual order ≤, ut = uxx + f(x, u), Φt(u0) = u(t, ·). X = R, f ր, x(n + 1) = f(x(n)), n ≥ 0, Φn(x(0)) = f (n)(x(0)).

standing assumptions: T = R+. ∀x ∈ X, {Φt(x) : t ≥ 0} has compact closure in X. H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 2 / 16

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Monotone Dynamical System

1

State space: metric space (X, d) with a closed* partial order relation ≤.

*(xn ≤ yn ∧ xn → x ∧ yn → y ⇒ x ≤ y) 2

Dynamics: discrete-time (T = Z+) or continuous-time (T = R+) semiflow Φ : T × X → X. Notation Φt(x) = Φ(t, x):

Φ continuous. Φ0 = idX Φt ◦ Φs = Φt+s, t, s ∈ T

3

Order-Preserving: x ≤ y ⇒ Φt(x) ≤ Φt(y), t ∈ T, x, y ∈ X.

Trivial Examples: X = R, usual order ≤, x′ = f(x), Φt(x0) = x(t, x0). X = BC(R, R), usual order ≤, ut = uxx + f(x, u), Φt(u0) = u(t, ·). X = R, f ր, x(n + 1) = f(x(n)), n ≥ 0, Φn(x(0)) = f (n)(x(0)).

standing assumptions: T = R+. ∀x ∈ X, {Φt(x) : t ≥ 0} has compact closure in X. H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 2 / 16

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Monotone Dynamical System

1

State space: metric space (X, d) with a closed* partial order relation ≤.

*(xn ≤ yn ∧ xn → x ∧ yn → y ⇒ x ≤ y) 2

Dynamics: discrete-time (T = Z+) or continuous-time (T = R+) semiflow Φ : T × X → X. Notation Φt(x) = Φ(t, x):

Φ continuous. Φ0 = idX Φt ◦ Φs = Φt+s, t, s ∈ T

3

Order-Preserving: x ≤ y ⇒ Φt(x) ≤ Φt(y), t ∈ T, x, y ∈ X.

Trivial Examples: X = R, usual order ≤, x′ = f(x), Φt(x0) = x(t, x0). X = BC(R, R), usual order ≤, ut = uxx + f(x, u), Φt(u0) = u(t, ·). X = R, f ր, x(n + 1) = f(x(n)), n ≥ 0, Φn(x(0)) = f (n)(x(0)).

standing assumptions: T = R+. ∀x ∈ X, {Φt(x) : t ≥ 0} has compact closure in X. H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 2 / 16

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Ordered Banach Space Induces ≤

X ⊂ Y, Y an ordered Banach space with closed positive cone Y+: (R+)Y+ ⊂ Y+, Y+ + Y+ ⊂ Y+, (Y+) ∩ (−Y+) = {0} Partial order: y ≤ x ⇔ x − y ∈ Y+ Y is strongly ordered if Int Y+ = ∅. Then y ≪ x ⇔ x − y ∈ Int Y+. Examples: Y = Rn, Y+ = Rk

+ × (−Rn−k +

), 0 ≤ k ≤ n : x ≤ y ⇔ (xi ≤ yi, i ≤ k) ∧ (xj ≥ yj, j > k) Y = Lp(Ω, Rn), Cr(Ω, Rn), f ≤ g ⇔ f(s) ≤ g(s), s ∈ Ω

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 3 / 16

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Ordered Banach Space Induces ≤

X ⊂ Y, Y an ordered Banach space with closed positive cone Y+: (R+)Y+ ⊂ Y+, Y+ + Y+ ⊂ Y+, (Y+) ∩ (−Y+) = {0} Partial order: y ≤ x ⇔ x − y ∈ Y+ Y is strongly ordered if Int Y+ = ∅. Then y ≪ x ⇔ x − y ∈ Int Y+. Examples: Y = Rn, Y+ = Rk

+ × (−Rn−k +

), 0 ≤ k ≤ n : x ≤ y ⇔ (xi ≤ yi, i ≤ k) ∧ (xj ≥ yj, j > k) Y = Lp(Ω, Rn), Cr(Ω, Rn), f ≤ g ⇔ f(s) ≤ g(s), s ∈ Ω

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 3 / 16

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Ordered Banach Space Induces ≤

X ⊂ Y, Y an ordered Banach space with closed positive cone Y+: (R+)Y+ ⊂ Y+, Y+ + Y+ ⊂ Y+, (Y+) ∩ (−Y+) = {0} Partial order: y ≤ x ⇔ x − y ∈ Y+ Y is strongly ordered if Int Y+ = ∅. Then y ≪ x ⇔ x − y ∈ Int Y+. Examples: Y = Rn, Y+ = Rk

+ × (−Rn−k +

), 0 ≤ k ≤ n : x ≤ y ⇔ (xi ≤ yi, i ≤ k) ∧ (xj ≥ yj, j > k) Y = Lp(Ω, Rn), Cr(Ω, Rn), f ≤ g ⇔ f(s) ≤ g(s), s ∈ Ω

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 3 / 16

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Equilibria, Sub & Super

Equilibria: E = {e ∈ X : ∀t ≥ 0, Φt(e) = e} Sub-equilibria: E− = {x ∈ X : ∀t ≥ 0, Φt(x) ≥ x} x ∈ E− ⇒ x ≤ Φs(x) ≤ Φt+s(x), t, s ≥ 0 ∴ Φt(x) ր e ∈ E, t ր ∞. Super-equilibria: {x ∈ X : ∀t ≥ 0, Φt(x) ≤ x}

in applications, these can be identified by the semiflow generator H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 4 / 16

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Equilibria, Sub & Super

Equilibria: E = {e ∈ X : ∀t ≥ 0, Φt(e) = e} Sub-equilibria: E− = {x ∈ X : ∀t ≥ 0, Φt(x) ≥ x} x ∈ E− ⇒ x ≤ Φs(x) ≤ Φt+s(x), t, s ≥ 0 ∴ Φt(x) ր e ∈ E, t ր ∞. Super-equilibria: {x ∈ X : ∀t ≥ 0, Φt(x) ≤ x}

in applications, these can be identified by the semiflow generator H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 4 / 16

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Equilibria, Sub & Super

Equilibria: E = {e ∈ X : ∀t ≥ 0, Φt(e) = e} Sub-equilibria: E− = {x ∈ X : ∀t ≥ 0, Φt(x) ≥ x} x ∈ E− ⇒ x ≤ Φs(x) ≤ Φt+s(x), t, s ≥ 0 ∴ Φt(x) ր e ∈ E, t ր ∞. Super-equilibria: {x ∈ X : ∀t ≥ 0, Φt(x) ≤ x}

in applications, these can be identified by the semiflow generator H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 4 / 16

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Equilibria, Sub & Super

Equilibria: E = {e ∈ X : ∀t ≥ 0, Φt(e) = e} Sub-equilibria: E− = {x ∈ X : ∀t ≥ 0, Φt(x) ≥ x} x ∈ E− ⇒ x ≤ Φs(x) ≤ Φt+s(x), t, s ≥ 0 ∴ Φt(x) ր e ∈ E, t ր ∞. Super-equilibria: {x ∈ X : ∀t ≥ 0, Φt(x) ≤ x}

in applications, these can be identified by the semiflow generator H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 4 / 16

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Sub & Super Equilibria Bracket Basin

x1 is a sub-equilibrium with Φt(x1) ր e ∈ E. Monotonicity implies B = {x ∈ X : x1 ≤ x ≤ e} ⊂ Basin of attraction of e because it is “sandwiched": Φt(x1) ≤ Φt(x) ≤ Φt(e) = e

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 5 / 16

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Strong Monotonicity & Limit Set Dichotomy

Φ strongly monotone (Hirsch) if Y is strongly ordered and x < y ⇒ Φt(x) ≪ Φt(y), t > 0. Φ is strongly order preserving (Matano) (SOP) if it is monotone and x < y ⇒ ∃ nbhds U, V, x ∈ U, y ∈ V, ∃ t0 ≥ 0 such that Φt0(U) ≤ Φt0(V) Theorem[LSD, Hirsch(1982)]: Let Φ be SOP . If x < y then either (a) ω(x) < ω(y), or (b) ω(x) = ω(y) ⊂ E

ω(x) = omega limit set of x H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 6 / 16

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Strong Monotonicity & Limit Set Dichotomy

Φ strongly monotone (Hirsch) if Y is strongly ordered and x < y ⇒ Φt(x) ≪ Φt(y), t > 0. Φ is strongly order preserving (Matano) (SOP) if it is monotone and x < y ⇒ ∃ nbhds U, V, x ∈ U, y ∈ V, ∃ t0 ≥ 0 such that Φt0(U) ≤ Φt0(V) Theorem[LSD, Hirsch(1982)]: Let Φ be SOP . If x < y then either (a) ω(x) < ω(y), or (b) ω(x) = ω(y) ⊂ E

ω(x) = omega limit set of x H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 6 / 16

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Generic Convergence

Theorem*: Assume X ⊂ Y, Y an ordered Banach space, and X is either convex or the closure of an open set. Let C = {x ∈ X : Φt(x) → e, e ∈ Equilibria} If Φ is SOP on X and some mild smoothness and compactness

assumptions hold (†), then Int C is dense in X.

*Inspired by: M. Hirsch. Systems of differential equations which are competitive or cooperative II: convergence almost everywhere, SIAM J. Math. Anal., 16, 1985. (†)∃τ > 0: x1 < x2 ⇒ Φτ x1 ≪ Φτ x2 Φτ is locally C1 at each e ∈ E, Φ′

τ (e) is Krein-Rutman operator.

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 7 / 16

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ODEs-A Canonical Form

x′ = F(x) is a monotone system w.r.t. orthant cone Rk

+ × (−Rn−k +

) in domain X if, on permuting variables x = (x1, x2), x1 ∈ Rk, x2 ∈ Rn−k x′

1

= f1(x1, x2) x′

2

= f2(x1, x2) diagonal blocks ∂fi

∂xi (x) have nonnegative off-diagonal entries.

  • ff-diagonal blocks ∂fi

∂xj (x) ≤ 0, i = j have nonpositive entries.

Jacobian =     ∗ + − − + ∗ − − − − ∗ + − − + ∗     , + ≥ 0, − ≤ 0

Components cluster into two subgroups. positive within-group interactions, negative between-group interactions. Strong monotonicity holds if the Jacobian is irreducible at a.e. x ∈ X!

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 8 / 16

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ODEs-A Canonical Form

x′ = F(x) is a monotone system w.r.t. orthant cone Rk

+ × (−Rn−k +

) in domain X if, on permuting variables x = (x1, x2), x1 ∈ Rk, x2 ∈ Rn−k x′

1

= f1(x1, x2) x′

2

= f2(x1, x2) diagonal blocks ∂fi

∂xi (x) have nonnegative off-diagonal entries.

  • ff-diagonal blocks ∂fi

∂xj (x) ≤ 0, i = j have nonpositive entries.

Jacobian =     ∗ + − − + ∗ − − − − ∗ + − − + ∗     , + ≥ 0, − ≤ 0

Components cluster into two subgroups. positive within-group interactions, negative between-group interactions. Strong monotonicity holds if the Jacobian is irreducible at a.e. x ∈ X!

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 8 / 16

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ODEs-A Canonical Form

x′ = F(x) is a monotone system w.r.t. orthant cone Rk

+ × (−Rn−k +

) in domain X if, on permuting variables x = (x1, x2), x1 ∈ Rk, x2 ∈ Rn−k x′

1

= f1(x1, x2) x′

2

= f2(x1, x2) diagonal blocks ∂fi

∂xi (x) have nonnegative off-diagonal entries.

  • ff-diagonal blocks ∂fi

∂xj (x) ≤ 0, i = j have nonpositive entries.

Jacobian =     ∗ + − − + ∗ − − − − ∗ + − − + ∗     , + ≥ 0, − ≤ 0

Components cluster into two subgroups. positive within-group interactions, negative between-group interactions. Strong monotonicity holds if the Jacobian is irreducible at a.e. x ∈ X!

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 8 / 16

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Repressilator with 2 genes

xi = [protein] product of gene i yi = [mRNA] of gene i. xi−1 represses transcription of yi: x′

i

= βi(yi − xi) y′

i

= αifi(xi−1) − yi, i = 1, 2, mod 2 where αi, βi > 0 and fi > 0 satisfies f ′

i < 0.

Jacobian =     − + − − − + − −    

Gardner et al, “Construction of a genetic toggle switch in E. coli", Nature(403),2000. H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 9 / 16

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Dynamics of Repressilator

Equilibria u = (x1, y1, x2, y2) are in 1-to-1 correspondence with fixed points of increasing map g ≡ α2f2 ◦ α1f1

0.5 1 1.5 2 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 x2 g(x2) Fixed Points of g

Theorem: If g has no degenerate fixed points, ∃ odd number of equilibria u1, u2, · · · , u2m+1 indexed by increasing values of x2. u2i+1 are stable, u2i are

  • unstable. If B(ui) denotes the basin of attraction of ui, then

∪odd iB(ui) is open and dense in R4

+. u1 is globally attracting if m = 0.

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 10 / 16

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Repressilator with transcription and translation delays

x′

i (t)

= βi[yi(t − µi) − xi(t)] y′

i (t)

= αifi(xi−1(t − τi−1)) − yi(t), i = 1, 2 Generates a SOP semiflow on: X = C([−τ1, 0], R+) × C([−µ1, 0], R+) ×C([−τ2, 0], R+) × C([−µ2, 0], R+) Previous Theorem holds without change for delayed repressilator. Extends to arbitrary even number of genes.

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 11 / 16

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Test for Orthant-Cone Monotone ODE x′ = f(x)

∀i = j,

∂fi ∂xj (x) does not change sign in X.

Feedback Symmetry: ∂fi

∂xj (x) ∂fj ∂xi (y) ≥ 0, i = j. golden rule

Construct signed, influence graph:

un-directed edge joins i to j = i if ∃x ∈ X,

∂fi ∂xj (x) = 0.

append + sign to edge if derivative is positive, − sign if negative.

balanced graph (‡): every loop (cycle) has even number of “−" signs.

‡ This is Harary’s Theorem: “a balanced network is clusterable". See “Networks: An Intro.", M. Newman An algorithm is given for clustering, i.e, permuting indices into subsets I = {1, 2, · · · , k} and Ic. H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 12 / 16

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Systems of Parabolic PDEs

Given elliptic operators Li, the parabolic system ∂tu1 = L1u1 + f1(x, u1, u2) ∂tu2 = L2u2 + f2(x, u1, u2), x ∈ Ω, t > 0 where f = (f1(x, ·, ·), f2(x, ·, ·)) in canonical form, and boundary conditions 0 = αi ∂ui ∂n + βiui, x ∈ ∂Ω where αi, βi ≥ 0, generates a monotone semiflow on spaces Cr

0(Ω) := {v ∈ Cr(Ω) : v|∂Ω = 0}

r = 0, 1 for Dirichlet B.C., or Cr

α,β(Ω) :=

  • v ∈ Cr(Ω) : βv + α∂v

∂n = 0, x ∈ ∂Ω

  • for Robin or Neumann B.C.

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 13 / 16

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Convergence to uniform equilibria

ut = D∇2u + f(u) ∂u ∂n = 0, x ∈ ∂Ω u(x, 0) = u0(x), x ∈ Ω Ω ⊂ Rn smooth, bounded, convex. D = diag(di), di > 0. f : Rm → Rm is C2, cooperative, and irreducible. Theorem[Enciso, Hirsch, S. (2008)]: Let solutions of u′ = f(u) be bounded on t ≥ 0. The set of u0 ∈ C(Ω, Rm) such that u(x, t) converges to a spatially-uniform equilibrium is prevalent in C(Ω, Rm).

W is prevalent if its complement is shy. Borel set W ⊂ X = C(Ω, Rm) is shy if ∃ a nonzero compactly supported Borel measure µ on X, such that µ(W + x) = 0, ∀x ∈ X. Hunt,Sauer,Yorke,1993 H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 14 / 16

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Unmentioned & New Directions

Monotone Maps: No LSD, generic convergence to periodic points. Non-autonomous theory-Skew-Product Semiflows: J. Mierczynski,

  • W. Shen, X. Zhao

Monotone Random Systems: See I. Chueshov, Springer Lect. Notes in Math. Control Theory: Sontag, Angeli, De Leenheer, Enciso, Wang

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 15 / 16

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My Favorite References

Monotone Dynamical Systems, H.S. & M. Hirsch, Handbook of Differential Equations , Ordinary Differential Equations ( volume 2), eds. A.Canada, P .Drabek, A.Fonda, Elsevier, 239-357, 2005. Monotone systems, a mini-review, H.S. & M.W. Hirsch, in Positive

  • Systems. Proceedings of the First Multidisciplinary Symposium on

Positive Systems (POSTA 2003). Luca Benvenuti, Alberto De Santis and Lorenzo Farina (Eds.) Lecture Notes on Control and Information Sciences vol. 294, Springer Verlag, Heidelberg, 2003. Monotone Maps: A Review, H.S.& M. Hirsch, J. Difference Eqns.& Appl. 11(2005) 379-398 Monotone Dynamical Systems: an introduction to the theory of competitive and cooperative systems, Amer. Math. Soc. Surveys and Monograghs, 41, 1995. Systems of ordinary differential equations which generate an order preserving flow. A survey of results, SIAM Review 30, 1988.

H.L. Smith (ASU) Monotone Dynamical Systems Sontagfest, May 23, 2011 16 / 16