26 May 2015 to 12 June 2015
Mainz Institute for Theoretical Physics<br>Johannes Gutenberg University
Europe/Berlin timezone

Zhegalkin zebra motives

29 May 2015, 11:00
45m
02.430 (Mainz Institute for Theoretical Physics<br>Johannes Gutenberg University)

02.430

Mainz Institute for Theoretical Physics<br>Johannes Gutenberg University

Staudingerweg 9 / 2<sup>nd</sup> floor 55128 Mainz

Speaker

Jan Stienstra

Description

A Zhegalkin polynomial in n variables is a polynomial function on {F_2}^n; here F_2={0,1} is the field with 2 elements. The zebra with frequency vector v is the F_2 - valued function Z on the plane R^2 defined by the formula Z(x) = floor(2v\cdot x) mod 2. By inserting an n-tuple of zebras into an n-variable Zhegalkin polynomial one obtains an F_2 - valued function F on R^2, which we call a Zhegalkin zebra function. The graph of such a function gives a partion of the plane into black (i.e. F=1) and white (i.e. F=0) areas. This easily produces many beautiful pictures. We will focus on examples for which the picture is a doubly periodic tiling of the plane by black and white convex polygons. These tilings have a very rich geometric structure (including so-called brane tilings or dimer models, Poisson structures, Calabi-Yau manifolds). We focus in particular on examples which reproduce the quantum-periods of the DelPezzo surfaces, and may therefore be considered as mirrors of DelPezzo surfaces.

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