Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:2309.16766 · Journal of High Energy Physics

An intuitive construction of modular flow

Jonathan Sorce

Published Dec 12, 2023• 18 citations
arXivHTMLPDF

Abstract

Abstract The theory of modular flow has proved extremely useful for applying thermodynamic reasoning to out-of-equilibrium states in quantum field theory. However, the standard proofs of the fundamental theorems of modular flow use machinery from Fourier analysis on Banach spaces, and as such are not especially transparent to an audience of physicists. In this article, I present a construction of modular flow that differs from existing treatments. The main pedagogical contribution is that I start with thermal physics via the KMS condition, and derive the modular operator as the only operator that could generate a thermal time-evolution map, rather than starting with the modular operator as the fundamental object of the theory. The main technical contribution is a new proof of the fundamental theorem stating that modular flow is a symmetry. The new proof circumvents the delicate issues of Fourier analysis that appear in previous treatments, but is still mathematically rigorous.

DOI
10.1007/jhep12(2023)079

Related papers

Resolving modular flow: a toolkit for free fermions

Johanna Erdmenger B, Pascal Fries, Ignacio A. Reyes +1 more

Abstract Modular flow is a symmetry of the algebra of observables associated to space-time regions. Being closely related to entanglement, it has played a key role in recent connections between information theory, QFT and gravity. However, little is known about its action beyond highly symmetric cases. The key idea of this work is to introduce a new formula for modular flows for free chiral fermions in 1 + 1 dimensions, working directly from the resolvent, a standard technique in complex analysis. We present novel results — not fixed by conformal symmetry — for disjoint regions on the plane, cylinder and torus. Depending on temperature and boundary conditions, these display different behaviour ranging from purely local to non-local in relation to the mixing of operators at spacelike separation. We find the modular two-point function, whose analytic structure is in precise agreement with the KMS condition that governs modular evolution. Our ready-to-use formulae may provide new ingredients to explore the connection between spacetime and entanglement.

arXiv:2008.07532•Journal of High Energy Physics•Dec 1, 2020•14 citations

Resolving modular flow: a toolkit for free fermions

Johanna Erdmenger B, Fries, P., Ignacio A. Reyes +1 more

Modular flow is a symmetry of the algebra of observables associated to spacetime regions. Being closely related to entanglement, it has played a key role in recent connections between information theory, QFT and gravity. However, little is known about its action beyond highly symmetric cases. The key idea of this work is to introduce a new formula for modular flows for free chiral fermions in $1+1$ dimensions, working directly from the \\textit{resolvent}, a standard technique in complex analysis. We present novel results -- not fixed by conformal symmetry -- for disjoint regions on the plane, cylinder and torus. Depending on temperature and boundary conditions, these display different behaviour ranging from purely local to non-local in relation to the mixing of operators at spacelike separation. We find the modular two-point function, whose analytic structure is in precise agreement with the KMS condition that governs modular evolution. Our ready-to-use formulae may provide new ingredients to explore the connection between spacetime and entanglement.

•Dec 21, 2020•13 citations

Quantum Temporal Order: Structural Inevitability of Modular Flow and the Problem of Time

Kishore K

We address the problem of time in quantum mechanics: time is an external classical parameter, not a quantum observable, yet quantum gravity requires it to be emergent. We show that a canonical preferred temporal flow arises from within the algebraic structure of quantum mechanics, without presupposing a Hamiltonian, a Schrödinger equation, or a background time parameter. The starting point is a pair (M, ω) — a von Neumann algebra of observables and a faithful normal state — with no other input. From these, Tomita–Takesaki modular theory derives a canonical strongly-continuous one-parameter group of automorphisms σ_t : M → M (the modular flow). The group parameter t labels the spectral flow of the modular operator Δ = S^*S constructed from ω, and is not assumed as background structure. Three results are established. First (Structural Inevitability): any non-tracial quantum system unavoidably carries a non-trivial modular flow — the Tomita–Takesaki modular automorphism group, derived from algebraic data alone. Under the Connes–Rovelli thermal time hypothesis (adopted as an explicit physical postulate, supported by exact agreement with Heisenberg evolution for Gibbs states and with Rindler time via the Bisognano–Wichmann theorem), this flow constitutes physical time. Second (Cocycle Colimit): the directed colimit of all subsystem modular flows exists in the category W*-Dyn, interacting or not; for interacting systems the colimit is twisted by Araki's Connes cocycle, and the assembled flow equals the modular flow of the limiting algebra. Third (Classical Recovery): a structural outline of how, in the decoherence limit under density, separability, and the second law, the framework recovers a separable dense linear order from which n-dimensional spatial structure is derived; full topological reconstruction is left as an open program. This paper is self-contained and requires no companion papers. It extends the Connes–Rovelli thermal time hypothesis and the Page–Wootters relational framework to a universal directed cocycle colimit.

•Mar 2, 2026•0 citations

An Algebraic Formulation of Thermality in Nested Rindler Wedges

Waheed A. Dar, Prince Ahmad Ganai, Nirmalya Kajuri

Padmanabhan and Kolekar had demonstrated the phenomenon of recursive thermality in two dimensional free field theories where the Rindler vacuum appears thermal to an observer accelerated with respect to the Rindler observer. We study the same construction at an algebraic level for conformal field theories. At each step, a parent wedge is conformally mapped to a reference Minkowski spacetime, where a new right Rindler wedge and its left sibling are selected. We illustrate that under the Bisognano--Wichmann property, thermality holds at every generation: the state associated with a parent wedge becomes a KMS state when restricted to its right child. Further, using the modular structure of the wedge and its causal sibling, we identify the sibling algebra with the modular commutant and derive the corresponding recursive modular flow explicitly.

arXiv:2610.27007•Oct 19, 2026•0 citations

Modular theory and affine representations on the Rindler horizon

Michele Arzano, Paolo Palumbo

We develop a group-theoretic interpretation of the Unruh effect based on affine symmetry on a light ray and relate it to modular theory. For a massless scalar field in two spacetime dimensions inertial and uniformly accelerated observers select two different flows within the same chiral one-particle structure, respectively, null translations and dilations. Minkowski modes are adapted to translations, while Rindler modes are adapted to dilations, with the Mellin transform providing the natural bridge between them. When a Minkowski positive-frequency mode is restricted to a single Rindler wedge, its comparison with Rindler modes is non-unitary within the positive-frequency sector. Modular theory gives the corresponding operator-algebraic interpretation: on the horizon the modular flow of the half-line algebra is implemented by dilations, and the restricted vacuum satisfies the KMS condition. The affine group thus appears as the minimal symmetry structure underlying thermality on the Rindler horizon.

hep-thCross-listedarXiv:2606.01071•Jun 2, 2026

Symmetry-resolved modular correlation functions in free fermionic theories

Giuseppe Di Giulio, Johanna Erdmenger B

Abstract As a new ingredient for analyzing the fine structure of entanglement, we study the symmetry resolution of the modular flow of U(1)-invariant operators in theories endowed with a global U(1) symmetry. We provide a consistent definition of symmetry-resolved modular flow that is defined for a local algebra of operators associated to a sector with fixed charge. We also discuss the symmetry-resolved modular correlation functions and show that they satisfy the KMS condition in each symmetry sector. Our analysis relies on the factorization of the Hilbert space associated to spatial subsystems. We provide a toolkit for computing the symmetry-resolved modular correlation function of the charge density operator in free fermionic theories. As an application, we compute this correlation function for a 1 + 1-dimensional free massless Dirac field theory and find that it is independent of the charge sector at leading order in the ultraviolet cutoff expansion. This feature can be regarded as a charge equipartition of the modular correlation function. Although obtained for free fermions, these results may be of potential interest for bulk reconstruction in AdS/CFT.

arXiv:2305.02343•Journal of High Energy Physics•Jul 6, 2023•15 citations
Abstract The theory of modular flow has proved extremely useful for applying thermodynamic reasoning to out-of-equilibrium states in quantum field theory. However, the standard proofs of the fundamental theorems of modular flow use machinery from Fourier analysis on Banach spaces, and as such are not especially transparent to an audience of physicists. In this article, I present a construction of modular flow that differs from existing treatments. The main pedagogical contribution is that I start with thermal physics via the KMS condition, and derive the modular operator as the only operator that could generate a thermal time-evolution map, rather than starting with the modular operator as the fundamental object of the theory. The main technical contribution is a new proof of the fundamental theorem stating that modular flow is a symmetry. The new proof circumvents the delicate issues of Fourier analysis that appear in previous treatments, but is still mathematically rigorous.
Abstract Modular flow is a symmetry of the algebra of observables associated to space-time regions. Being closely related to entanglement, it has played a key role in recent connections between information theory, QFT and gravity. However, little is known about its action beyond highly symmetric cases. The key idea of this work is to introduce a new formula for modular flows for free chiral fermions in 1 + 1 dimensions, working directly from the resolvent, a standard technique in complex analysis. We present novel results — not fixed by conformal symmetry — for disjoint regions on the plane, cylinder and torus. Depending on temperature and boundary conditions, these display different behaviour ranging from purely local to non-local in relation to the mixing of operators at spacelike separation. We find the modular two-point function, whose analytic structure is in precise agreement with the KMS condition that governs modular evolution. Our ready-to-use formulae may provide new ingredients to explore the connection between spacetime and entanglement.
Modular flow is a symmetry of the algebra of observables associated to spacetime regions. Being closely related to entanglement, it has played a key role in recent connections between information theory, QFT and gravity. However, little is known about its action beyond highly symmetric cases. The key idea of this work is to introduce a new formula for modular flows for free chiral fermions in 1+11+11+1 dimensions, working directly from the \\textit{resolvent}, a standard technique in complex analysis. We present novel results -- not fixed by conformal symmetry -- for disjoint regions on the plane, cylinder and torus. Depending on temperature and boundary conditions, these display different behaviour ranging from purely local to non-local in relation to the mixing of operators at spacelike separation. We find the modular two-point function, whose analytic structure is in precise agreement with the KMS condition that governs modular evolution. Our ready-to-use formulae may provide new ingredients to explore the connection between spacetime and entanglement.
We address the problem of time in quantum mechanics: time is an external classical parameter, not a quantum observable, yet quantum gravity requires it to be emergent. We show that a canonical preferred temporal flow arises from within the algebraic structure of quantum mechanics, without presupposing a Hamiltonian, a Schrödinger equation, or a background time parameter. The starting point is a pair (M, ω) — a von Neumann algebra of observables and a faithful normal state — with no other input. From these, Tomita–Takesaki modular theory derives a canonical strongly-continuous one-parameter group of automorphisms σ_t : M → M (the modular flow). The group parameter t labels the spectral flow of the modular operator Δ = S^*S constructed from ω, and is not assumed as background structure. Three results are established. First (Structural Inevitability): any non-tracial quantum system unavoidably carries a non-trivial modular flow — the Tomita–Takesaki modular automorphism group, derived from algebraic data alone. Under the Connes–Rovelli thermal time hypothesis (adopted as an explicit physical postulate, supported by exact agreement with Heisenberg evolution for Gibbs states and with Rindler time via the Bisognano–Wichmann theorem), this flow constitutes physical time. Second (Cocycle Colimit): the directed colimit of all subsystem modular flows exists in the category W*-Dyn, interacting or not; for interacting systems the colimit is twisted by Araki's Connes cocycle, and the assembled flow equals the modular flow of the limiting algebra. Third (Classical Recovery): a structural outline of how, in the decoherence limit under density, separability, and the second law, the framework recovers a separable dense linear order from which n-dimensional spatial structure is derived; full topological reconstruction is left as an open program. This paper is self-contained and requires no companion papers. It extends the Connes–Rovelli thermal time hypothesis and the Page–Wootters relational framework to a universal directed cocycle colimit.
Padmanabhan and Kolekar had demonstrated the phenomenon of recursive thermality in two dimensional free field theories where the Rindler vacuum appears thermal to an observer accelerated with respect to the Rindler observer. We study the same construction at an algebraic level for conformal field theories. At each step, a parent wedge is conformally mapped to a reference Minkowski spacetime, where a new right Rindler wedge and its left sibling are selected. We illustrate that under the Bisognano--Wichmann property, thermality holds at every generation: the state associated with a parent wedge becomes a KMS state when restricted to its right child. Further, using the modular structure of the wedge and its causal sibling, we identify the sibling algebra with the modular commutant and derive the corresponding recursive modular flow explicitly.
We develop a group-theoretic interpretation of the Unruh effect based on affine symmetry on a light ray and relate it to modular theory. For a massless scalar field in two spacetime dimensions inertial and uniformly accelerated observers select two different flows within the same chiral one-particle structure, respectively, null translations and dilations. Minkowski modes are adapted to translations, while Rindler modes are adapted to dilations, with the Mellin transform providing the natural bridge between them. When a Minkowski positive-frequency mode is restricted to a single Rindler wedge, its comparison with Rindler modes is non-unitary within the positive-frequency sector. Modular theory gives the corresponding operator-algebraic interpretation: on the horizon the modular flow of the half-line algebra is implemented by dilations, and the restricted vacuum satisfies the KMS condition. The affine group thus appears as the minimal symmetry structure underlying thermality on the Rindler horizon.
Abstract As a new ingredient for analyzing the fine structure of entanglement, we study the symmetry resolution of the modular flow of U(1)-invariant operators in theories endowed with a global U(1) symmetry. We provide a consistent definition of symmetry-resolved modular flow that is defined for a local algebra of operators associated to a sector with fixed charge. We also discuss the symmetry-resolved modular correlation functions and show that they satisfy the KMS condition in each symmetry sector. Our analysis relies on the factorization of the Hilbert space associated to spatial subsystems. We provide a toolkit for computing the symmetry-resolved modular correlation function of the charge density operator in free fermionic theories. As an application, we compute this correlation function for a 1 + 1-dimensional free massless Dirac field theory and find that it is independent of the charge sector at leading order in the ultraviolet cutoff expansion. This feature can be regarded as a charge equipartition of the modular correlation function. Although obtained for free fermions, these results may be of potential interest for bulk reconstruction in AdS/CFT.