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On operator growth and emergent Poincaré symmetries

Javier M. Magan, Joan Simon

TL;DR

The paper analyzes operator growth in generic large-N gauge theories at finite temperature by decomposing operators into Fourier modes that evolve without mixing, demonstrating that leading-order dynamics are fixed by two-point functions. It shows how an emergent bulk Poincaré algebra arises in holographic theories via doubled boundary/operator algebras (Rindler-like construction) and mirror operators, linking operator growth to near-horizon symmetries. The authors unify various growth notions (size, number/energy measures, recursion method, and quantum complexity) within the GNS formalism, arguing that, at large-N, these notions reduce to functionals of two-point data and thus are equivalent on both sides of holography. They also connect operator growth to quantum chaos and discuss how Minkowski energy growth yields Lyapunov behavior, with implications for chaos in AdS/CFT and the interpretation of bulk infalling physics.

Abstract

We consider operator growth for generic large-N gauge theories at finite temperature. Our analysis is performed in terms of Fourier modes, which do not mix with other operators as time evolves, and whose correlation functions are determined by their two-point functions alone, at leading order in the large-N limit. The algebra of these modes allows for a simple analysis of the operators with whom the initial operator mixes over time, and guarantees the existence of boundary CFT operators closing the bulk Poincaré algebra, describing the experience of infalling observers. We discuss several existing approaches to operator growth, such as number operators, proper energies, the many-body recursion method, quantum circuit complexity, and comment on its relation to classical chaos in black hole dynamics. The analysis evades the bulk vs boundary dichotomy and shows that all such approaches are the same at both sides of the holographic duality, a statement that simply rests on the equality between operator evolution itself. In the way, we show all these approaches have a natural formulation in terms of the Gelfand-Naimark-Segal (GNS) construction, which maps operator evolution to a more conventional quantum state evolution, and provides an extension of the notion of operator growth to QFT.

On operator growth and emergent Poincaré symmetries

TL;DR

The paper analyzes operator growth in generic large-N gauge theories at finite temperature by decomposing operators into Fourier modes that evolve without mixing, demonstrating that leading-order dynamics are fixed by two-point functions. It shows how an emergent bulk Poincaré algebra arises in holographic theories via doubled boundary/operator algebras (Rindler-like construction) and mirror operators, linking operator growth to near-horizon symmetries. The authors unify various growth notions (size, number/energy measures, recursion method, and quantum complexity) within the GNS formalism, arguing that, at large-N, these notions reduce to functionals of two-point data and thus are equivalent on both sides of holography. They also connect operator growth to quantum chaos and discuss how Minkowski energy growth yields Lyapunov behavior, with implications for chaos in AdS/CFT and the interpretation of bulk infalling physics.

Abstract

We consider operator growth for generic large-N gauge theories at finite temperature. Our analysis is performed in terms of Fourier modes, which do not mix with other operators as time evolves, and whose correlation functions are determined by their two-point functions alone, at leading order in the large-N limit. The algebra of these modes allows for a simple analysis of the operators with whom the initial operator mixes over time, and guarantees the existence of boundary CFT operators closing the bulk Poincaré algebra, describing the experience of infalling observers. We discuss several existing approaches to operator growth, such as number operators, proper energies, the many-body recursion method, quantum circuit complexity, and comment on its relation to classical chaos in black hole dynamics. The analysis evades the bulk vs boundary dichotomy and shows that all such approaches are the same at both sides of the holographic duality, a statement that simply rests on the equality between operator evolution itself. In the way, we show all these approaches have a natural formulation in terms of the Gelfand-Naimark-Segal (GNS) construction, which maps operator evolution to a more conventional quantum state evolution, and provides an extension of the notion of operator growth to QFT.

Paper Structure

This paper contains 25 sections, 147 equations.