{"paper":{"title":"Nonlocal Nonstabilizerness from Holographic Schwinger Pair Production","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Holographic calculation shows that Schwinger quark pairs dynamically generate nonlocal magic when spacetime dimension exceeds two.","cross_cats":["gr-qc","hep-ph","nucl-th","quant-ph"],"primary_cat":"hep-th","authors_text":"Sebastian Grieninger","submitted_at":"2026-05-05T18:48:47Z","abstract_excerpt":"We analyze the emergence of nonlocal magic in Schwinger pair creation in strong non-Abelian (chromo)electric fields using holography. The produced quark--antiquark pair is entangled into a color singlet, yet accelerates into causally disconnected Rindler wedges. Using the Casini--Huerta--Myers conformal mapping and the probe-brane framework, we compute the refined R\\'enyi entropy and its derivative, which captures the antiflatness of the entanglement spectrum for a spherical bipartition. We find that for boundary spacetime dimension $d>2$, the entanglement spectrum is non-flat, implying the dy"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We find that for boundary spacetime dimension d>2, the entanglement spectrum is non-flat, implying the dynamical generation of nonlocal magic in the pair creation process.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The Casini-Huerta-Myers conformal mapping together with the probe-brane framework in the holographic dual accurately captures the nonlocal aspects of the entanglement spectrum for the accelerating Schwinger pair.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Holographic Schwinger pair creation generates nonlocal magic for spacetime dimensions d>2, as shown by a non-flat entanglement spectrum that can be read from the probe brane free energy.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Holographic calculation shows that Schwinger quark pairs dynamically generate nonlocal magic when spacetime dimension exceeds two.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"67df6c50d7ded575f46375b5fd78411c4c3b1837b8762741187f44c357611ec6"},"source":{"id":"2605.04210","kind":"arxiv","version":2},"verdict":{"id":"4507d4f8-df01-4dd6-8c88-b6545315df3c","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-08T17:26:11.389845Z","strongest_claim":"We find that for boundary spacetime dimension d>2, the entanglement spectrum is non-flat, implying the dynamical generation of nonlocal magic in the pair creation process.","one_line_summary":"Holographic Schwinger pair creation generates nonlocal magic for spacetime dimensions d>2, as shown by a non-flat entanglement spectrum that can be read from the probe brane free energy.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The Casini-Huerta-Myers conformal mapping together with the probe-brane framework in the holographic dual accurately captures the nonlocal aspects of the entanglement spectrum for the accelerating Schwinger pair.","pith_extraction_headline":"Holographic calculation shows that Schwinger quark pairs dynamically generate nonlocal magic when spacetime dimension exceeds two."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.04210/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"ai_meta_artifact","ran_at":"2026-05-20T12:36:28.592211Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T23:31:21.101890Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T14:42:12.011866Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"bb83456e119b4dba04ccb3c050b4aa056e06fb75815de13c44f2cf11e2c9d66e"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}