Progress Report D. Parker, M. Puljiz, J. E. Rowe UoB Maths Misc. - - PowerPoint PPT Presentation

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Progress Report D. Parker, M. Puljiz, J. E. Rowe UoB Maths Misc. - - PowerPoint PPT Presentation

UoB Maths C. Good, N. Kamaleson, C. Mu, Progress Report D. Parker, M. Puljiz, J. E. Rowe UoB Maths Misc. Problem 1 University of Birmingham Problem 2 Chris Good, Nishanthan Kamaleson, Chunyan Mu, References David Parker, Mate Puljiz,


slide-1
SLIDE 1

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Progress Report UoB Maths

University of Birmingham Chris Good, Nishanthan Kamaleson, Chunyan Mu, David Parker, Mate Puljiz, Jonathan E. Rowe Birmingham, 29th April 2015

slide-2
SLIDE 2

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Lattices for Lagrange interpolation

Recall: Finding a valid linear coarse graining = Finding a common invariant subspace of the differential DT|x Jacobi - Evaluate at random points If we know that T is a polynomial then e.g. Ben Yaacov and also Chung, Yao give sets of points that suffices to check

slide-3
SLIDE 3

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Frobenius theorem, Integrability, Foliations

Continuous time dynamics on a manifold ˙ x = F(x) regular1 coarse grainings correspond to foliations Theorem (Frobenius’ theorem) A subbundle E is integrable if and only if it arises from a regular foliation of M. (Dimension of leaves + Dimension of E = Dimension of M) Taking F as the subbundle, FT gives a sufficient condition for existence of coarse graining onto a 1 dimensional manifold, projecting perpendicular to F

1level sets are manifolds of constant dimension

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SLIDE 4

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Integrability condition on F is d F ∧ F = 0 E.g. in R3 this amounts to requiring (∇ × F) · F = 0 But what about CG that aren’t perpendicular to F? The extensions seem plausible (and possibly already known).

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SLIDE 5

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Dense periodic points in cellular automata

Alphabet A = {1, 2, . . . , n} The full shift ΣA = AZ The shift map σ : ΣA → ΣA σ((ξi)i) = (ξi+1)i A cellular automaton is a continuous σ-commuting map F : ΣA → ΣA. Equivalently ∃k ∈ N and Φ : A2k+1 → A s.t. (F((ξi)i))j = Φ(ξj−k, . . . ξj+k)

slide-6
SLIDE 6

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

’It is an open problem whether all surjective CA, or at least all transitive CA, have a dense set of properly periodic points.’ Blanchard Consider the coarse graining π : ΣA → ΣA2k+1 which arranges entries of ξ in groups of 2k + 1 It follows that π conjugates F on ΣA to a cellular automaton G on ΣA2k+1 but G has depth k = 1. F is surjective/has periodic points dense iff G is surjective/has periodic points dense

slide-7
SLIDE 7

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Reaction networks

Organisation theory

  • rganisation = closed + self-maintaining

Theorem (Dittrich et al.) Given an ODE ˙ x = Sv(x), the abstraction of the stationary state (which is usually attracting) is an organisation. Can this be extended?

slide-8
SLIDE 8

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

The replicator equation (see in Fontana, Buss) ˙ xi =

  • j
  • k

ai

j,kxjxk − xi

  • r,s,t

at

r,sxrxs

What about its stationary state? Higher order equations? Relation to the heuristic framework?

slide-9
SLIDE 9

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

Connections with other papers

Rabitz et al. [’89-’97] study Kinetic differential equations, their lumpings and stability Equations studied are exactly the replicator equations and higher order analogues

slide-10
SLIDE 10

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

References I

[1] Walter Fontana and Leo W Buss, The arrival of the fittest: Toward a theory of biological organization, Bulletin of Mathematical Biology 56 (1994), no. 1, 1–64. [2] Peter Dittrich and Pietro Speroni Di Fenizio, Chemical organisation theory, Bulletin of mathematical biology 69 (2007), no. 4, 1199–1231. [3] Alison S Tomlin, Genyuan Li, Herschel Rabitz, and J´ anos T´

  • th, The

effect of lumping and expanding on kinetic differential equations, SIAM Journal on Applied Mathematics 57 (1997), no. 6, 1531–1556. [4] Genyuan Li and Herschel Rabitz, A general analysis of approximate lumping in chemical kinetics, Chemical engineering science 45 (1990),

  • no. 4, 977–1002.
slide-11
SLIDE 11

UoB Maths

  • C. Good,
  • N. Kamaleson,
  • C. Mu,
  • D. Parker,
  • M. Puljiz,
  • J. E. Rowe

Misc. Problem 1 Problem 2 References

References II

[5] Genyuan Li, Herschel Rabitz, and J´ anos T´

  • th, A general analysis of

exact nonlinear lumping in chemical kinetics, Chemical Engineering Science 49 (1994), no. 3, 343–361. [6] K. C. Chung and T. H. Yao, On lattices admitting unique Lagrange interpolations, SIAM J. Numer. Anal. 14 (1977), no. 4, 735–743. MR0445158 (56 #3502) [7] Ita¨ ı Ben Yaacov, A multivariate version of the Vandermonde determinant identity, arXiv:1405.0993 (2014). [8] http: //www.encyclopediaofmath.org/index.php/Pfaffian_equation [9] https://www.math.iupui.edu/˜mmisiure/open/FB1.pdf