Universality M. Hairer University of Warwick New fellows seminar - - PowerPoint PPT Presentation

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Universality M. Hairer University of Warwick New fellows seminar - - PowerPoint PPT Presentation

Universality M. Hairer University of Warwick New fellows seminar Universality Experimental / numerical fact: large-scale behaviour of systems displaying random behaviour self-similar and independent of microscopic description. Universality


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Universality

  • M. Hairer

University of Warwick

New fellows seminar

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Universality

Experimental / numerical fact: large-scale behaviour of systems displaying random behaviour self-similar and independent of microscopic description.

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Universality

Experimental / numerical fact: large-scale behaviour of systems displaying random behaviour self-similar and independent of microscopic description. Example: Random walks / central limit theorem

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Universality

Experimental / numerical fact: large-scale behaviour of systems displaying random behaviour self-similar and independent of microscopic description. Example: Surface growth (KPZ)

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Universality

Experimental / numerical fact: large-scale behaviour of systems displaying random behaviour self-similar and independent of microscopic description. Example: Surface growth (KPZ)

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Heuristic explanation

Schematic evolution in “space of models” under rescaling: Want to understand these “fixed points” and this picture! Fixed points are universal scale-invariant models. Mathematically tractable when fixed point is Gaussian, very hard

  • therwise. (Conformal invariance helps a lot in 2D.)
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Heuristic explanation

Schematic evolution in “space of models” under rescaling: Want to understand these “fixed points” and this picture! Fixed points are universal scale-invariant models. Mathematically tractable when fixed point is Gaussian, very hard

  • therwise. (Conformal invariance helps a lot in 2D.)
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Heuristic explanation

Schematic evolution in “space of models” under rescaling: Want to understand these “fixed points” and this picture! Fixed points are universal scale-invariant models. Mathematically tractable when fixed point is Gaussian, very hard

  • therwise. (Conformal invariance helps a lot in 2D.)
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Intermediate situation

Sometimes Gaussian and non-Gaussian fixed points coexist. Schematic evolution under rescaling: G N Can we understand red line and blue region? Weaker form of universality.

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Intermediate situation

Sometimes Gaussian and non-Gaussian fixed points coexist. Schematic evolution under rescaling: G N Can we understand red line and blue region? Weaker form of universality.

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Interface fluctuation models

Gaussian fixed point: Edwards-Wilkinson universality class. Exponents 1/2 in space and 1/4 in time. Gaussian fluctuations with explicit description. Nonlinear fixed point: KPZ universality class. Exponents 2/3 in space and 1/3 in time. Fluctuations described by random matrix (Tracy-Widom) distributions. No full description yet. Crossover regime: (red line) KPZ equation: ∂th = ∂2

xh + (∂xh)2 + ξ .

Behaves like EW at small scales and KPZ at large scales. Recent contribution: build robust solution theory allowing to show universality results.

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Interface fluctuation models

Gaussian fixed point: Edwards-Wilkinson universality class. Exponents 1/2 in space and 1/4 in time. Gaussian fluctuations with explicit description. Nonlinear fixed point: KPZ universality class. Exponents 2/3 in space and 1/3 in time. Fluctuations described by random matrix (Tracy-Widom) distributions. No full description yet. Crossover regime: (red line) KPZ equation: ∂th = ∂2

xh + (∂xh)2 + ξ .

Behaves like EW at small scales and KPZ at large scales. Recent contribution: build robust solution theory allowing to show universality results.

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Interface fluctuation models

Gaussian fixed point: Edwards-Wilkinson universality class. Exponents 1/2 in space and 1/4 in time. Gaussian fluctuations with explicit description. Nonlinear fixed point: KPZ universality class. Exponents 2/3 in space and 1/3 in time. Fluctuations described by random matrix (Tracy-Widom) distributions. No full description yet. Crossover regime: (red line) KPZ equation: ∂th = ∂2

xh + (∂xh)2 + ξ .

Behaves like EW at small scales and KPZ at large scales. Recent contribution: build robust solution theory allowing to show universality results.

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Main problem

Problem: Functions are not smooth. Usual definition of smoothness: Obviously bad idea!

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Main problem

Problem: Functions are not smooth. Usual definition of smoothness: Obviously bad idea!

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Main problem

Problem: Functions are not smooth. Usual definition of smoothness: Obviously bad idea!

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Main problem

Problem: Functions are not smooth. Usual definition of smoothness: Obviously bad idea!

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A possible solution

Main idea: construct purpose-built objects and describe solution in terms of these: Problem of ill-posed operations boils down to constructing them at the level of these objects.

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A possible solution

Main idea: construct purpose-built objects and describe solution in terms of these: Problem of ill-posed operations boils down to constructing them at the level of these objects.