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  <title><![CDATA[PhD Defense by Han Liang]]></title>
  <body><![CDATA[<p><strong>School of Physics Thesis Dissertation Defense</strong></p><p>&nbsp;</p><p><strong>Han Liang</strong><br>Advisor: Dr. Predrag Cvitanović,&nbsp;School of Physics, Georgia Institute&nbsp;of Technology&nbsp;</p><p><br><strong>A Deterministic Lattice Field Theory of Spatiotemporal Chaos</strong></p><p>Date: Monday, May 12, 2025<br>Time: 1:00 p.m.<br>Location: Howey N201/N202<br><br><strong>Zoom link</strong>: &nbsp;<a href="https://gatech.zoom.us/j/98851319184">https://gatech.zoom.us/j/98851319184</a></p><p>&nbsp;</p><p><br><strong>Committee members:</strong><br>Dr. Elisabetta Matsumoto, &nbsp;School of Physics, Georgia Institute&nbsp;of Technology</p><p>Dr. Martin Mourigal, &nbsp;School of Physics, Georgia Institute&nbsp;of Technology</p><p>Dr. Zeb Rocklin, School of Physics, Georgia Institute of Technology<br>Dr. Luca Dieci, School of Mathematics, Georgia Institute of Technology</p><p><br><strong>Abstract:</strong><br>Traditional periodic orbit theory enables the evaluation of statistical properties of finite-dimensional chaotic dynamical systems through the</p><p>hierarchy of their periodic orbits. However, this approach becomes impractical for spatiotemporally chaotic systems over large or infinite</p><p>spatial domains. As the spatial extents of these systems increase, the physical dimensions grow linearly, requiring exponentially more distinct</p><p>periodic orbits to describe the dynamics to the same accuracy. To address this challenge, we propose a novel approach, describing spatiotemporally</p><p>chaotic or turbulent systems using the chaotic field theories discretized over multi-dimensional spatiotemporal lattices. The `chaos theory' is</p><p>here recast in the language of statistical mechanics, field theory, and solid state physics, with traditional periodic orbit theory of</p><p>low-dimensional, temporally chaotic dynamics a special, one-dimensional case.</p><p>&nbsp;</p><p>In this field-theoretical formulation, there is no time evolution. Instead, by treating the temporal and spatial directions on equal footing,</p><p>one determines the spatiotemporally periodic states that contribute to the theory's partition function, each a solution of the system's</p><p>deterministic defining equations, with sums over time-periodic orbits of dynamical systems theory now replaced by sums of d-periodic states over</p><p>d-dimensional spacetime geometries, weighted by their global orbit stabilities.</p><p>&nbsp;</p><p>The orbit stability of each periodic state is evaluated using the determinant of its spatiotemporal orbit Jacobian matrix. We derive the</p><p>Hill's formula, which relates the global orbit stability to the conventional low-dimensional forward-in-time evolution stability, and</p><p>show that the field-theoretical formulation is equivalent to the temporal periodic orbit theory for systems with fixed finite spatial extent. By</p><p>summing the partition functions over different spacetime geometries, we extend the temporal periodic orbit theory to spatiotemporal systems. The</p><p>multiple periodicities of spatiotemporally periodic states are described in the language of crystallography using Bravais lattices. Applying the</p><p>Floquet-Bloch theorem to evaluate the spectrum of orbit Jacobian operators of periodic states, we compute their multiplicative weights, leading to</p><p>the spatiotemporal zeta function formulation of the theory in terms of prime orbits. Hyperbolic shadowing of periodic orbits by pseudo orbits</p><p>ensures that the predictions of the theory are dominated by the prime periodic orbits with shortest spatiotemporal periods.</p><p>&nbsp;</p><p>&nbsp;</p>]]></body>
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