{"paper":{"title":"Momentum-space entanglement and mutual information in Kaluza-Klein reduction","arxiv_id":"2610.37009","primary_cat":"hep-th","submitted_at":"2026-10-27T10:52:00+00:00","version_compiled":"v1"},"notice":"Every quoted sentence is the authors' text from the arXiv listing abstract. Labels and probabilities are the outputs of classifier-1.13.0 on the question bank abstract-p1-20260923, exactly as returned. No sentence in this record was written by a language model.","schema":"pith.compiled-record/v0","status":"compiled","abstract":{"source":"arXiv listing abstract v1","sentences":[{"i":0,"p":1.0,"id":"s0","own":false,"role":"background","text":"In theories with compact extra dimensions, the four-dimensional effective description is obtained by Kaluza-Klein reduction.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.04,"main_claim_p":0.02,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":1.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":1,"p":0.99,"id":"s1","own":false,"role":"background","text":"The state available to a four-dimensional observer is the reduced density matrix obtained by tracing the higher-dimensional vacuum over the tower of massive modes, and it need not be pure.","hedge":{"p":0.69,"label":"asserted"},"own_p":0.09,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.0,"background":0.99,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":2,"p":1.0,"id":"s2","own":true,"role":"contribution","text":"In this paper we study the momentum-space entanglement of this state for a five-dimensional scalar on $M_4\\times S^1$ with a cubic or quartic self-interaction.","hedge":{"p":0.95,"label":"asserted"},"own_p":0.82,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.21,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":1.0,"interpretation":0.0}},{"i":3,"p":0.73,"id":"s3","own":true,"role":"contribution","text":"We compute, at leading order in the coupling, the mutual information $I_n$ between the zero modes below a resolution scale $\\mu$ and a single Kaluza-Klein level $n$.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.96,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.2,"role_probabilities":{"gap":0.0,"method":0.26,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.73,"interpretation":0.0}},{"i":4,"p":1.0,"id":"s4","own":true,"role":"result","text":"When the zero modes couple linearly and without derivatives to pairs of tower modes, $I_n$ falls as $1/m_n$, where $m_n$ is the mass of level $n$.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.89,"main_claim_p":0.13,"quantitative":true,"quantitative_p":0.84,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":5,"p":1.0,"id":"s5","own":true,"role":"result","text":"In the cubic theory, this tail is independent of the ultraviolet cutoff, with coefficient $(\\mu R)^2/1024\\pi^3$ for compactification radius $R$, and the mutual information with the whole tower grows logarithmically with the number of levels.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.18,"quantitative":true,"quantitative_p":0.98,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":6,"p":1.0,"id":"s6","own":true,"role":"result","text":"In the quartic theory, the tail is masked by states containing additional hard quanta, which make $I_n$ depend on the cutoff.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.9,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":7,"p":0.93,"id":"s7","own":true,"role":"interpretation","text":"Compared with the corrections the tower makes to low-energy amplitudes, which are dominated by the lightest levels and captured by local operators, the mutual information with the tower is not dominated by any finite set of levels and arises from the time-nonlocal part of the effective action.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.79,"main_claim_p":0.42,"quantitative":true,"quantitative_p":0.7,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.07,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.93}},{"i":8,"p":0.99,"id":"s8","own":true,"role":"interpretation","text":"The local four-dimensional effective theory therefore describes the low-energy observables of the reduced system but not its state.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.66,"main_claim_p":0.54,"quantitative":false,"quantitative_p":0.13,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.99}},{"i":9,"p":0.85,"id":"s9","own":true,"role":"result","text":"Unbroken supersymmetry cancels the vacuum energy of the compactification but not the mutual information, which at leading order is a sum of squared amplitudes.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.68,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.27,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.85,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.14}}]},"compiled":{"main_claim":{"p":0.96,"text":"The local four-dimensional effective theory therefore describes the low-energy observables of the reduced system but not its state.","location":"abstract s8","hedge_strength":{"p":1.0,"label":"asserted"}},"provenance":{"route":{"via":"TypeSafe API","model":"classifier-1.13.0","endpoint":"https://api.typesafe.ai/v1/systemone","provider":"TypeSafe"},"packing":"one request per 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