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This paper advances foundational quantum field theory by rigorously defining the relationship between Haag duality and causal-complement channel classes using algebraic frameworks like von Neumann algebras. It establishes quantitative invariants linking commutativity defects to spacelike separation, offering precise mathematical bounds for bosonic nets that are critical for understanding fundamental limits in relativistic quantum information processing.
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Essential Duality and Maximal Non-signalling Extensions in Algebraic Quantum Field Theory

arXiv2 min read

arXiv:2605.00075v2 Announce Type: replace Abstract: Let \(O\mapsto A(O)\) be a local Haag--Kastler net and let \(A^d(O)=A(O')'\) be its dual net. Normal unital completely positive maps on \(B(H)\) that fix \(A(O')\) pointwise are exactly the channels with Kraus operators in \(A^d(O)\). Thus Haag duality at \(O\) is equivalent to equality with the \(A(O)\)-inner channels, while essential duality is equivalent to order-independence of the corresponding causal-complement channel classes at spacelike separation. For self-adjoint generators \(a\in M\) and \(b\in N\), the small-parameter order defect has coefficient \(\operatorname{diam}\sigma(-i[a,b])\). Uniform optimization gives \(\Gamma(M,N)=2\Delta_{\mathrm{sa}}(M,N)\), and reversible inner-channel cb balls recover the same invariant through \(\lim_{\varepsilon\downarrow0}\Omega^{\mathrm{rev}}_\varepsilon(M,N)/\varepsilon^2=\Gamma(M,N)/4\). The full inner-channel class admits a normalized coefficient with the same commutativity zero set. With a positive reference observable \(G\), the mean-input-energy-constrained coefficient \(\Gamma_{G,E}\) has the same zero criterion and increases to \(\Gamma\) as \(E\to\infty\), while no model-independent recovery rate follows from the general von Neumann-algebraic hypotheses. For bosonic second-quantization nets the spacelike defect is either \(0\) or \(4\); generalized free-field examples realize both branches. In the translation-covariant case with positive one-particle time generator, failure of essential duality admits extremal bounded witness flows that are energy-limited relative to the second-quantized time-translation energy.

Abstract:Let \(O\mapsto A(O)\) be a local Haag--Kastler net and let \(A^d(O)=A(O')'\) be its dual net. Normal unital completely positive maps on \(B(H)\) that fix \(A(O')\) pointwise are exactly the channels with Kraus operators in \(A^d(O)\). Thus Haag duality at \(O\) is equivalent to equality with the \(A(O)\)-inner channels, while essential duality is equivalent to order-independence of the corresponding causal-complement channel classes at spacelike separation. For self-adjoint generators \(a\in M\) and \(b\in N\), the small-parameter order defect has coefficient \(\operatorname{diam}\sigma(-i[a,b])\). Uniform optimization gives \(\Gamma(M,N)=2\Delta_{\mathrm{sa}}(M,N)\), and reversible inner-channel cb balls recover the same invariant through \(\lim_{\varepsilon\downarrow0}\Omega^{\mathrm{rev}}_\varepsilon(M,N)/\varepsilon^2=\Gamma(M,N)/4\). The full inner-channel class admits a normalized coefficient with the same commutativity zero set. With a positive reference observable \(G\), the mean-input-energy-constrained coefficient \(\Gamma_{G,E}\) has the same zero criterion and increases to \(\Gamma\) as \(E\to\infty\), while no model-independent recovery rate follows from the general von Neumann-algebraic hypotheses. For bosonic second-quantization nets the spacelike defect is either \(0\) or \(4\); generalized free-field examples realize both branches. In the translation-covariant case with positive one-particle time generator, failure of essential duality admits extremal bounded witness flows that are energy-limited relative to the second-quantized time-translation energy.

28 pages, no figures. Substantially revised version. Corrects the distinction between Haag and essential duality, replaces the earlier maximal-extension formulation by the channel-order framework, and adds quantitative, energy-constrained, and second-quantization results

arXiv:2605.00075 [quant-ph]

(or arXiv:2605.00075v2 [quant-ph] for this version)

Full text under the publisher's open licence · 225 words

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