{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WCDYZ4N5QSKXREDAPQQEFYDFYJ","short_pith_number":"pith:WCDYZ4N5","schema_version":"1.0","canonical_sha256":"b0878cf1bd84957890607c2042e065c271f6b87b69bb7bc27d7129b19322988f","source":{"kind":"arxiv","id":"1410.7289","version":3},"attestation_state":"computed","paper":{"title":"The infrared problem in QED: A lesson from a model with Coulomb interaction and realistic photon emission","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"F. Strocchi, G. Morchio","submitted_at":"2014-10-27T16:08:13Z","abstract_excerpt":"The scattering of photons and heavy classical Coulomb interacting particles, with realistic particle-photon interaction (without particle recoil) is studied adopting the Koopman formulation for the particles. The model is translation invariant and allows for a complete control of the Dollard strategy devised by Kulish-Faddeev and Rohrlich (KFR) for QED: in the adiabatic formulation, the M{\\o}ller operators exist as strong limits and interpolate between the dynamics and a non-free asymptotic dynamics, which is a unitary group; the $S$-matrix is non-trivial and exhibits the factorization of all "},"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":"1410.7289","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-27T16:08:13Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"9999add11f614725d89d6b0bf9a24cbd97d590331f11dcda8758ba49bec29928","abstract_canon_sha256":"134a8e59f2ee40d07f7f4aa5b03608701a77421dfc39d97536d70d16232ae905"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:08.268033Z","signature_b64":"q+5UT7P3CX6+qCOkrwTU/lEpeIKur7V9v5YrATyIArdwcZLip3ykxwMEXkQUtwddWudJdIjrqkkHjeT+JOs2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0878cf1bd84957890607c2042e065c271f6b87b69bb7bc27d7129b19322988f","last_reissued_at":"2026-05-18T01:30:08.267455Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:08.267455Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The infrared problem in QED: A lesson from a model with Coulomb interaction and realistic photon emission","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"F. Strocchi, G. Morchio","submitted_at":"2014-10-27T16:08:13Z","abstract_excerpt":"The scattering of photons and heavy classical Coulomb interacting particles, with realistic particle-photon interaction (without particle recoil) is studied adopting the Koopman formulation for the particles. The model is translation invariant and allows for a complete control of the Dollard strategy devised by Kulish-Faddeev and Rohrlich (KFR) for QED: in the adiabatic formulation, the M{\\o}ller operators exist as strong limits and interpolate between the dynamics and a non-free asymptotic dynamics, which is a unitary group; the $S$-matrix is non-trivial and exhibits the factorization of all "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.7289","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1410.7289","created_at":"2026-05-18T01:30:08.267544+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.7289v3","created_at":"2026-05-18T01:30:08.267544+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.7289","created_at":"2026-05-18T01:30:08.267544+00:00"},{"alias_kind":"pith_short_12","alias_value":"WCDYZ4N5QSKX","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WCDYZ4N5QSKXREDA","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WCDYZ4N5","created_at":"2026-05-18T12:28:54.890064+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ","json":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ.json","graph_json":"https://pith.science/api/pith-number/WCDYZ4N5QSKXREDAPQQEFYDFYJ/graph.json","events_json":"https://pith.science/api/pith-number/WCDYZ4N5QSKXREDAPQQEFYDFYJ/events.json","paper":"https://pith.science/paper/WCDYZ4N5"},"agent_actions":{"view_html":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ","download_json":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ.json","view_paper":"https://pith.science/paper/WCDYZ4N5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.7289&json=true","fetch_graph":"https://pith.science/api/pith-number/WCDYZ4N5QSKXREDAPQQEFYDFYJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WCDYZ4N5QSKXREDAPQQEFYDFYJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ/action/storage_attestation","attest_author":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ/action/author_attestation","sign_citation":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ/action/citation_signature","submit_replication":"https://pith.science/pith/WCDYZ4N5QSKXREDAPQQEFYDFYJ/action/replication_record"}},"created_at":"2026-05-18T01:30:08.267544+00:00","updated_at":"2026-05-18T01:30:08.267544+00:00"}