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arXiv:2610.40874

Proof of the entropic ccc-theorem

Jonah Kudler-Flam

hep-thcond-mat.str-elmath-phquant-phSubmitted Oct 29, 2026• Announced Nov 2, 2026
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Abstract

We prove an entropic $c$-theorem in two dimensions by constructing a $c$-function from the mutual information between spacelike separated wedges, defined through the relative entropy. The proof follows Casini and Huerta's, with strong subadditivity of entanglement entropy replaced by increasing differences of the mutual information, which we prove directly in the continuum from the split property and standard properties of relative entropy. The benefit of relative entropy is that every quantity we use is finite and no cutoff ever needs to be introduced. The assumptions of the theorem are only the standard axioms of algebraic quantum field theory, the split property with finite mutual information across a gap (both implied by modular $p$-nuclearity), and a finite ultraviolet bound on the resulting $c$-functions. We also note that, formally, the $c$-function is proportional to the minimal averaged null energy of a state that reproduces the vacuum correlations between the two wedges.

AI Summary

The paper asks whether the two-dimensional entropic $c$-theorem can be proved directly in continuum quantum field theory, without introducing ultraviolet-regulated entanglement entropies. It replaces entropy strong subadditivity with an increasing-differences inequality for mutual information defined through relative entropy. For spacelike-separated wedges $L_a$ and $R_b$, potential infrared divergences are handled by defining $\mathcal D_R(a,A;b)=\sup_{Y\subset R_b}[I(L_a:Y)-I(L_A:Y)]$, with $Y$ a bounded causal diamond, and an analogous left-moving quantity. The resulting functions $C_R=6a\,\partial_A\mathcal D_R|_{A=a}$ and $C_L$ depend only on $r=\sqrt{ab}$ and are nonnegative and nonincreasing. Assumptions include the Haag–Kastler axioms, split inclusions with finite mutual information across bounded-region gaps, and finite ultraviolet bounds $\mathcal D_R\le(c_R^{\rm UV}/6)\log(A/a)$ and its left-moving counterpart. The proof establishes increasing differences using type-I approximations, the relative-entropy chain rule and monotonicity; additivity and boost invariance then reduce monotonicity to concavity of a one-variable function. At dilation-invariant fixed points, both functions are constant. For chiral-product conformal theories and finite-index rational extensions, $C_{R,L}=6\kappa_{R,L}$, where $\kappa$ is the leading adjacent-interval mutual-information logarithmic coefficient. Equality with stress-tensor central charges remains conditional in general, with rigorous identification available for a subclass. The ultraviolet and infrared limits are not proved to equal the corresponding limiting fixed-point values. A connection to the minimum averaged null energy required to reproduce wedge correlations is stated formally.

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We prove an entropic ccc-theorem in two dimensions by constructing a ccc-function from the mutual information between spacelike separated wedges, defined through the relative entropy. The proof follows Casini and Huerta's, with strong subadditivity of entanglement entropy replaced by increasing differences of the mutual information, which we prove directly in the continuum from the split property and standard properties of relative entropy. The benefit of relative entropy is that every quantity we use is finite and no cutoff ever needs to be introduced. The assumptions of the theorem are only the standard axioms of algebraic quantum field theory, the split property with finite mutual information across a gap (both implied by modular ppp-nuclearity), and a finite ultraviolet bound on the resulting ccc-functions. We also note that, formally, the ccc-function is proportional to the minimal averaged null energy of a state that reproduces the vacuum correlations between the two wedges.
The paper asks whether the two-dimensional entropic ccc-theorem can be proved directly in continuum quantum field theory, without introducing ultraviolet-regulated entanglement entropies. It replaces entropy strong subadditivity with an increasing-differences inequality for mutual information defined through relative entropy.
For spacelike-separated wedges LaL_aLa​ and RbR_bRb​, potential infrared divergences are handled by defining DR(a,A;b)=sup⁡Y⊂Rb[I(La:Y)−I(LA:Y)]\mathcal D_R(a,A;b)=\sup_{Y\subset R_b}[I(L_a:Y)-I(L_A:Y)]DR​(a,A;b)=supY⊂Rb​​[I(La​:Y)−I(LA​:Y)], with YYY a bounded causal diamond, and an analogous left-moving quantity. The resulting functions CR=6a ∂ADR∣A=aC_R=6a\,\partial_A\mathcal D_R|_{A=a}CR​=6a∂A​DR​∣A=a​ and CLC_LCL​ depend only on r=abr=\sqrt{ab}r=ab​ and are nonnegative and nonincreasing. Assumptions include the Haag–Kastler axioms, split inclusions with finite mutual information across bounded-region gaps, and finite ultraviolet bounds DR≤(cRUV/6)log⁡(A/a)\mathcal D_R\le(c_R^{\rm UV}/6)\log(A/a)DR​≤(cRUV​/6)log(A/a) and its left-moving counterpart. The proof establishes increasing differences using type-I approximations, the relative-entropy chain rule and monotonicity; additivity and boost invariance then reduce monotonicity to concavity of a one-variable function.
At dilation-invariant fixed points, both functions are constant. For chiral-product conformal theories and finite-index rational extensions, CR,L=6κR,LC_{R,L}=6\kappa_{R,L}CR,L​=6κR,L​, where κ\kappaκ is the leading adjacent-interval mutual-information logarithmic coefficient. Equality with stress-tensor central charges remains conditional in general, with rigorous identification available for a subclass. The ultraviolet and infrared limits are not proved to equal the corresponding limiting fixed-point values. A connection to the minimum averaged null energy required to reproduce wedge correlations is stated formally.
Abstract We derive the property of strong superadditivity of mutual information arising from the Markov property of the vacuum state in a conformal field theory and strong subadditivity of entanglement entropy. We show this inequality encodes unitarity bounds for different types of fields. These unitarity bounds are precisely the ones that saturate for free fields. This has a natural explanation in terms of the possibility of localizing algebras on null surfaces. A particular continuity property of mutual information characterizes free fields from the entropic point of view. We derive a general formula for the leading long distance term of the mutual information for regions of arbitrary shape which involves the modular flow of these regions. We obtain the general form of this leading term for two spheres with arbitrary orientations in spacetime, and for primary fields of any tensor representation. For free fields we further obtain the explicit form of the leading term for arbitrary regions with boundaries on null cones.
We derive the property of strong superadditivity of mutual information arising from the Markov property of the vacuum state in a conformal field theory and strong subadditivity of entanglement entropy. We show this inequality encodes unitarity bounds for different types of fields. These unitarity bounds are precisely the ones that saturate for free fields. This has a natural explanation in terms of the possibility of localizing algebras on null surfaces. A particular continuity property of mutual information characterizes free fields from the entropic point of view. We derive a general formula for the leading long distance term of the mutual information for regions of arbitrary shape which involves the modular flow of these regions. We obtain the general form of this leading term for two spheres with arbitrary orientations in spacetime, and for primary fields of any tensor representation. For free fields we further obtain the explicit form of the leading term for arbitrary regions with boundaries on null cones.
The trace over the degrees of freedom located in a subset of the space transforms the vacuum state into a mixed density matrix with nonzero entropy. This is usually called entanglement entropy, and it is known to be divergent in quantum field theory (QFT). However, it is possible to define a finite quantity F(A,B) for two given different subsets A and B which measures the degree of entanglement between their respective degrees of freedom. We show that the function F(A,B) is severely constrained by the Poincaré symmetry and the mathematical properties of the entropy. In particular, for one component sets in two-dimensional conformal field theories its general form is completely determined. Moreover, it allows to prove an alternative entropic version of the c-theorem for (1+1)-dimensional QFT. We propose this well-defined quantity as the meaningfull entanglement entropy and comment on possible applications in QFT and the black hole evaporation problem.
We study entanglement entropy (EE) for a Maxwell field in (2+1)(2+1)(2+1) dimensions. We do numerical calculations in two-dimensional lattices. This gives a concrete example of the general results of our recent work [1] on entropy for lattice gauge fields using an algebraic approach. To evaluate the entropies we extend the standard calculation methods for the entropy of Gaussian states in canonical commutation algebras to the more general case of algebras with center and arbitrary numerical commutators. We find that while the entropy depends on the details of the algebra choice, mutual information has a well defined continuum limit as predicted in [1]. We study several universal terms for the entropy of the Maxwell field and compare with the case of a massless scalar field. We find some interesting new phenomena: an ``evanescent'' logarithmically divergent term in the entropy with topological coefficient which does not have any correspondence with ultraviolet entanglement in the universal quantities, and a nonstandard way in which strong subadditivity is realized. Based on the results of our calculations we propose a generalization of strong subadditivity for the entropy on some algebras that are not in tensor product.
In the framework of Algebraic Quantum Field Theory, several operator algebraic notions of entanglement entropy can be associated with any pair of causally disjoint spacetime regions SA\mathcal{S}_ASA​ and SB\mathcal{S}_BSB​ with positive relative distance. Among them, the canonical entanglement entropy is defined as the von Neumann entropy of a canonical intermediate type I factor. In this work, we show that the canonical entanglement entropy of the vacuum state is finite for a broad class of conformal nets including the U(1)U(1)U(1)-current model and the SU(n)SU(n)SU(n)-loop group models. Since previous studies suggest that this finiteness property is related to nuclearity properties of the system, we show that the mutual information is finite in any local QFT satisfying a modular ppp-nuclearity condition for some 0<p<10 < p < 10<p<1. A similar finiteness result is established for another notion of entanglement entropy introduced in this paper. We conclude with remarks for future work in this direction.
We consider the problem of defining the entanglement entropy for chiral nets in the framework of algebraic quantum field theory.Considering a Möbius covariant local net with the split property, we give a sensible definition for the entropy H E I of a state restricted to a local algebra of an open connected non-dense interval I ⊂ S 1 , with a given "conformal energy cutoff E".Considering the vacuum state restricted to any such interval, we prove that the latter is finite, and we give some upper bound estimates in terms of the dimensions of eigenspaces of the conformal Hamiltonian.This thesis is based on a joint work with Yoh Tanimoto.