{"paper":{"title":"Quantum Gravity Beyond the Bulk","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"The generator of time evolution in quantum gravity reduces to a boundary charge at spatial infinity for external observers.","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Jorge Gamboa, Natalia Tapia-Arellano","submitted_at":"2026-05-14T16:21:56Z","abstract_excerpt":"We propose an infrared and asymptotic formulation of quantum gravity adapted to external observers. In an asymptotic proper-time gauge, the physical generator of evolution reduces to the Regge--Teitelboim boundary charge, so that quantum dynamics is governed by infrared gravitational configurations at spatial infinity. In the weak-field regime this leads naturally to a Born--Oppenheimer separation between slow asymptotic data and fast bulk fluctuations. Integrating out the latter induces a Berry connection on the space of admissible configurations, whose holonomy characterizes infrared-dressed"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"In an asymptotic proper-time gauge, the physical generator of evolution reduces to the Regge--Teitelboim boundary charge, so that quantum dynamics is governed by infrared gravitational configurations at spatial infinity.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The assumption that a Born-Oppenheimer separation between slow asymptotic data and fast bulk fluctuations is valid and that integrating out the latter produces a well-defined Berry connection without uncontrolled back-reaction or loss of unitarity.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Proposes reducing quantum gravity dynamics to Regge-Teitelboim boundary charges in an asymptotic proper-time gauge, yielding a Berry-phase effective Hamiltonian after integrating out bulk modes.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"The generator of time evolution in quantum gravity reduces to a boundary charge at spatial infinity for external observers.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"272e7e6f072176cde14d868898b57d6ebd86683c85c5f8411966060d5a5e9b7f"},"source":{"id":"2605.15251","kind":"arxiv","version":1},"verdict":{"id":"9759f1f7-d9dc-45ab-a1c9-9163daf3c7ef","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T16:19:26.029349Z","strongest_claim":"In an asymptotic proper-time gauge, the physical generator of evolution reduces to the Regge--Teitelboim boundary charge, so that quantum dynamics is governed by infrared gravitational configurations at spatial infinity.","one_line_summary":"Proposes reducing quantum gravity dynamics to Regge-Teitelboim boundary charges in an asymptotic proper-time gauge, yielding a Berry-phase effective Hamiltonian after integrating out bulk modes.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The assumption that a Born-Oppenheimer separation between slow asymptotic data and fast bulk fluctuations is valid and that integrating out the latter produces a well-defined Berry connection without uncontrolled back-reaction or loss of unitarity.","pith_extraction_headline":"The generator of time evolution in quantum gravity reduces to a boundary charge at spatial infinity for external observers."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.15251/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"doi_title_agreement","ran_at":"2026-05-19T16:31:18.434713Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T16:27:10.673365Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T15:01:54.143343Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.816798Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"a02ee9f46da975f97763dd5147b74925fd8c676959c60d16c74e308e50dcd49e"},"references":{"count":25,"sample":[{"doi":"10.1007/978-1-4612-4728-9","year":1987,"title":"J. 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