{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:RIZNTECPW5NV5535BP7X3UZVJI","short_pith_number":"pith:RIZNTECP","schema_version":"1.0","canonical_sha256":"8a32d9904fb75b5ef77d0bff7dd3354a2957b5190cf8c6af29bc458ab80649e4","source":{"kind":"arxiv","id":"1901.01454","version":1},"attestation_state":"computed","paper":{"title":"Catching p via s wave with indirect detection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","astro-ph.HE"],"primary_cat":"hep-ph","authors_text":"Bhaskar Dutta, James B. Dent, Louis E. Strigari, Steven J. Clark","submitted_at":"2019-01-05T18:31:04Z","abstract_excerpt":"For many dark matter models, the annihilation cross section to two-body final states is difficult to probe with current experiments because the dominant annihilation channel is velocity or helicity suppressed. The inclusion of gauge boson radiation for three-body final states can lift the helicity suppression, allowing a velocity-independent cross section to dominate the annihilation process, and providing an avenue to constrain these models. Here we examine experimental constraints on dark matter that annihilates to two leptons plus a bremsstrahlung boson, $\\bar{\\ell}+\\ell+\\gamma/W/Z$. We con"},"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":"1901.01454","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-01-05T18:31:04Z","cross_cats_sorted":["astro-ph.CO","astro-ph.HE"],"title_canon_sha256":"e9392eef0f37218e2d2af12de843b70310b03f442d3c80a802ed3d7aeb6f04c0","abstract_canon_sha256":"2087074f6d1a8d97becb3b17e90f7f31b8ed063c61a2d0150345fdf0f62307aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:30.996430Z","signature_b64":"MfQ5IFtr6JoGQ6fUwHu8hYVEF+s2qnG9QnyiWYgR8htq58tHoPBQJrQgOJeiMHQtMoULHsJ6F7X1P2qUOu7GBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a32d9904fb75b5ef77d0bff7dd3354a2957b5190cf8c6af29bc458ab80649e4","last_reissued_at":"2026-05-17T23:48:30.995933Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:30.995933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Catching p via s wave with indirect detection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","astro-ph.HE"],"primary_cat":"hep-ph","authors_text":"Bhaskar Dutta, James B. Dent, Louis E. Strigari, Steven J. Clark","submitted_at":"2019-01-05T18:31:04Z","abstract_excerpt":"For many dark matter models, the annihilation cross section to two-body final states is difficult to probe with current experiments because the dominant annihilation channel is velocity or helicity suppressed. The inclusion of gauge boson radiation for three-body final states can lift the helicity suppression, allowing a velocity-independent cross section to dominate the annihilation process, and providing an avenue to constrain these models. Here we examine experimental constraints on dark matter that annihilates to two leptons plus a bremsstrahlung boson, $\\bar{\\ell}+\\ell+\\gamma/W/Z$. We con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.01454","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":""},"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":"1901.01454","created_at":"2026-05-17T23:48:30.995989+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.01454v1","created_at":"2026-05-17T23:48:30.995989+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.01454","created_at":"2026-05-17T23:48:30.995989+00:00"},{"alias_kind":"pith_short_12","alias_value":"RIZNTECPW5NV","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_16","alias_value":"RIZNTECPW5NV5535","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_8","alias_value":"RIZNTECP","created_at":"2026-05-18T12:33:27.125529+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/RIZNTECPW5NV5535BP7X3UZVJI","json":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI.json","graph_json":"https://pith.science/api/pith-number/RIZNTECPW5NV5535BP7X3UZVJI/graph.json","events_json":"https://pith.science/api/pith-number/RIZNTECPW5NV5535BP7X3UZVJI/events.json","paper":"https://pith.science/paper/RIZNTECP"},"agent_actions":{"view_html":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI","download_json":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI.json","view_paper":"https://pith.science/paper/RIZNTECP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.01454&json=true","fetch_graph":"https://pith.science/api/pith-number/RIZNTECPW5NV5535BP7X3UZVJI/graph.json","fetch_events":"https://pith.science/api/pith-number/RIZNTECPW5NV5535BP7X3UZVJI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI/action/storage_attestation","attest_author":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI/action/author_attestation","sign_citation":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI/action/citation_signature","submit_replication":"https://pith.science/pith/RIZNTECPW5NV5535BP7X3UZVJI/action/replication_record"}},"created_at":"2026-05-17T23:48:30.995989+00:00","updated_at":"2026-05-17T23:48:30.995989+00:00"}