{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:RS63ACWIXMOZQWC67EZQWEP4G2","short_pith_number":"pith:RS63ACWI","schema_version":"1.0","canonical_sha256":"8cbdb00ac8bb1d98585ef9330b11fc368f83d169a63ace61159d3834cb59fb4d","source":{"kind":"arxiv","id":"2405.02222","version":2},"attestation_state":"computed","paper":{"title":"Unitarity in the non-relativistic regime and implications for dark matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Kalliopi Petraki, Marcos M. Flores","submitted_at":"2024-05-03T16:28:20Z","abstract_excerpt":"Unitarity sets upper limits on partial-wave elastic and inelastic cross-sections, which are often violated by perturbative computations. We discuss the dynamics underlying these limits in the non-relativistic regime, namely long-range interactions, and show how the resummation of the 2-particle-irreducible diagrams arising from squaring inelastic processes unitarizes both elastic and inelastic cross-sections. We provide a simple prescription to obtain the unitarized cross-sections from those that do not include resummation of the squared inelastic processes. Our results are model-independent, "},"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":"2405.02222","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-03T16:28:20Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"dcc238b5711f4f806f9e314c4f66dd59856c7f7f6c9058dfee752774e20563c2","abstract_canon_sha256":"eed3daa06cd4889b53afd77f80fcf014630412720258152b373b03a642739656"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:09:22.081825Z","signature_b64":"odJPub8F3qQC376bt+cReg/oPKAKG8brxzZLjrmjSpZPXlSseztAoA37+URfUVZH9Nzi9KtPm3vupjaX5DOqAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cbdb00ac8bb1d98585ef9330b11fc368f83d169a63ace61159d3834cb59fb4d","last_reissued_at":"2026-07-05T09:09:22.081310Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:09:22.081310Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unitarity in the non-relativistic regime and implications for dark matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Kalliopi Petraki, Marcos M. Flores","submitted_at":"2024-05-03T16:28:20Z","abstract_excerpt":"Unitarity sets upper limits on partial-wave elastic and inelastic cross-sections, which are often violated by perturbative computations. We discuss the dynamics underlying these limits in the non-relativistic regime, namely long-range interactions, and show how the resummation of the 2-particle-irreducible diagrams arising from squaring inelastic processes unitarizes both elastic and inelastic cross-sections. We provide a simple prescription to obtain the unitarized cross-sections from those that do not include resummation of the squared inelastic processes. Our results are model-independent, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.02222","kind":"arxiv","version":2},"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/2405.02222/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":"2405.02222","created_at":"2026-07-05T09:09:22.081378+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.02222v2","created_at":"2026-07-05T09:09:22.081378+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.02222","created_at":"2026-07-05T09:09:22.081378+00:00"},{"alias_kind":"pith_short_12","alias_value":"RS63ACWIXMOZ","created_at":"2026-07-05T09:09:22.081378+00:00"},{"alias_kind":"pith_short_16","alias_value":"RS63ACWIXMOZQWC6","created_at":"2026-07-05T09:09:22.081378+00:00"},{"alias_kind":"pith_short_8","alias_value":"RS63ACWI","created_at":"2026-07-05T09:09:22.081378+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.09686","citing_title":"Asymmetric Reheating of Dark QED","ref_index":67,"is_internal_anchor":false},{"citing_arxiv_id":"2605.05309","citing_title":"On the equivalence of unitarization prescriptions for the Sommerfeld enhancement","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11553","citing_title":"Self-consistent computation of pair production from non-relativistic effective field theories in the Keldysh-Schwinger formalism","ref_index":22,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2","json":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2.json","graph_json":"https://pith.science/api/pith-number/RS63ACWIXMOZQWC67EZQWEP4G2/graph.json","events_json":"https://pith.science/api/pith-number/RS63ACWIXMOZQWC67EZQWEP4G2/events.json","paper":"https://pith.science/paper/RS63ACWI"},"agent_actions":{"view_html":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2","download_json":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2.json","view_paper":"https://pith.science/paper/RS63ACWI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.02222&json=true","fetch_graph":"https://pith.science/api/pith-number/RS63ACWIXMOZQWC67EZQWEP4G2/graph.json","fetch_events":"https://pith.science/api/pith-number/RS63ACWIXMOZQWC67EZQWEP4G2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2/action/storage_attestation","attest_author":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2/action/author_attestation","sign_citation":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2/action/citation_signature","submit_replication":"https://pith.science/pith/RS63ACWIXMOZQWC67EZQWEP4G2/action/replication_record"}},"created_at":"2026-07-05T09:09:22.081378+00:00","updated_at":"2026-07-05T09:09:22.081378+00:00"}