{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:L5E4OUL6F5TPYQNFXRHMYNE57A","short_pith_number":"pith:L5E4OUL6","schema_version":"1.0","canonical_sha256":"5f49c7517e2f66fc41a5bc4ecc349df8353116ef26ef5ddd2328c19e3d536ee6","source":{"kind":"arxiv","id":"2606.27498","version":1},"attestation_state":"computed","paper":{"title":"Soft QED as Open Quantum System: Infrared Cancellation and Soft-Shell Coarse Graining","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-ph","quant-ph"],"primary_cat":"hep-th","authors_text":"Soo-Jong Rey","submitted_at":"2026-06-25T19:32:28Z","abstract_excerpt":"I formulate unresolved soft-photon sector of QED as open quantum system. Resolved charged particles and hard photons form the system, unresolved soft photons form the environment, and basic object is the reduced density matrix. A resolved outcome $f$ of multiple hard particles and photons has probability $P_{f}(i) =\\sum_n|\\langle f,n|S|i,0\\rangle|^2=\\langle i|F_f|i\\rangle$, with Kraus operators $K_n= {}_{\\rm soft} \\langle n|S|0 \\rangle_{\\rm soft}$ and effect $F_f=\\sum_nK_n^\\dagger\\Pi_fK_n$. The SK formulation places unresolved virtual and real terms in one doubled-contour expansion. At one loo"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2606.27498","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-25T19:32:28Z","cross_cats_sorted":["cond-mat.stat-mech","hep-ph","quant-ph"],"title_canon_sha256":"551e3a85afa0d6944926b319bb2ccefd7783c223d8a57c3798f977c2ef9de045","abstract_canon_sha256":"98c6f44ae16f4ab75b601409218879a6e7d6ca93f020101390ded9a6c7a783a1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-29T00:14:08.263333Z","signature_b64":"8QfUuGMFeyc/bGdpcjwrDFl0pIk/cDRjlC/FVV6CXiGqOk1tYOSm36wX6qf9UYx7QVO7YMXelamMiUf36cBICg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f49c7517e2f66fc41a5bc4ecc349df8353116ef26ef5ddd2328c19e3d536ee6","last_reissued_at":"2026-06-29T00:14:08.262928Z","signature_status":"signed_v1","first_computed_at":"2026-06-29T00:14:08.262928Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Soft QED as Open Quantum System: Infrared Cancellation and Soft-Shell Coarse Graining","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-ph","quant-ph"],"primary_cat":"hep-th","authors_text":"Soo-Jong Rey","submitted_at":"2026-06-25T19:32:28Z","abstract_excerpt":"I formulate unresolved soft-photon sector of QED as open quantum system. Resolved charged particles and hard photons form the system, unresolved soft photons form the environment, and basic object is the reduced density matrix. A resolved outcome $f$ of multiple hard particles and photons has probability $P_{f}(i) =\\sum_n|\\langle f,n|S|i,0\\rangle|^2=\\langle i|F_f|i\\rangle$, with Kraus operators $K_n= {}_{\\rm soft} \\langle n|S|0 \\rangle_{\\rm soft}$ and effect $F_f=\\sum_nK_n^\\dagger\\Pi_fK_n$. The SK formulation places unresolved virtual and real terms in one doubled-contour expansion. At one loo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.27498","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2606.27498/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2606.27498","created_at":"2026-06-29T00:14:08.262985+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.27498v1","created_at":"2026-06-29T00:14:08.262985+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.27498","created_at":"2026-06-29T00:14:08.262985+00:00"},{"alias_kind":"pith_short_12","alias_value":"L5E4OUL6F5TP","created_at":"2026-06-29T00:14:08.262985+00:00"},{"alias_kind":"pith_short_16","alias_value":"L5E4OUL6F5TPYQNF","created_at":"2026-06-29T00:14:08.262985+00:00"},{"alias_kind":"pith_short_8","alias_value":"L5E4OUL6","created_at":"2026-06-29T00:14:08.262985+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.01221","citing_title":"Type IIB Axion--Dilaton Wormholes and the BPS Limit Hessian","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2606.29804","citing_title":"Infrared Safety from ZX-Diagrams: A Categorical Proof of Soft-QED as Open Quantum System","ref_index":14,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A","json":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A.json","graph_json":"https://pith.science/api/pith-number/L5E4OUL6F5TPYQNFXRHMYNE57A/graph.json","events_json":"https://pith.science/api/pith-number/L5E4OUL6F5TPYQNFXRHMYNE57A/events.json","paper":"https://pith.science/paper/L5E4OUL6"},"agent_actions":{"view_html":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A","download_json":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A.json","view_paper":"https://pith.science/paper/L5E4OUL6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.27498&json=true","fetch_graph":"https://pith.science/api/pith-number/L5E4OUL6F5TPYQNFXRHMYNE57A/graph.json","fetch_events":"https://pith.science/api/pith-number/L5E4OUL6F5TPYQNFXRHMYNE57A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A/action/storage_attestation","attest_author":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A/action/author_attestation","sign_citation":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A/action/citation_signature","submit_replication":"https://pith.science/pith/L5E4OUL6F5TPYQNFXRHMYNE57A/action/replication_record"}},"created_at":"2026-06-29T00:14:08.262985+00:00","updated_at":"2026-06-29T00:14:08.262985+00:00"}