{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:YPYVKXUUTLWK55MM6KFNS4KDKM","short_pith_number":"pith:YPYVKXUU","schema_version":"1.0","canonical_sha256":"c3f1555e949aecaef58cf28ad97143530d3a689f1c6b51bd940f379db38f436c","source":{"kind":"arxiv","id":"1705.01633","version":1},"attestation_state":"computed","paper":{"title":"Validity of the Weizs\\\"acker-Williams Approximation and the Analysis of Beam Dump Experiments: Production of an axion, a dark photon, or a new axial-vector boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Gerald A. Miller, Yu-Sheng Liu","submitted_at":"2017-05-03T21:27:39Z","abstract_excerpt":"Beam dump experiments have been used to search for new particles, $\\phi$, with null results interpreted in terms of limits on masses $m_\\phi$ and coupling constants $\\epsilon$. However these limits have been obtained by using approximations [including the Weizs\\\"{a}cker-Williams (WW) approximation] or Monte-Carlo simulations. We display methods to obtain the cross section and the resulting particle production rates without using approximations on the phase space integral or Monte-Carlo simulations. In our previous work we examined the case of the new scalar boson production; in this paper we e"},"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":"1705.01633","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-03T21:27:39Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"e058610cc696eb744548630b2a9fc55cbcdc0c7e7d710d504209937f11e1c7b3","abstract_canon_sha256":"4d09bafdd565598b7babe073bb6d0ed4cf59716aa5f01e80a5a1c6aea4ef5d28"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:03.779504Z","signature_b64":"QUQQsIO00J9+DXff5cKaBTTxbTXpF/+BxrFoxByy+KF9hvKnxlVYDjniGvqT02LWaBXGK7c0KA1a5uShnWzJAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3f1555e949aecaef58cf28ad97143530d3a689f1c6b51bd940f379db38f436c","last_reissued_at":"2026-05-18T00:40:03.778805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:03.778805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Validity of the Weizs\\\"acker-Williams Approximation and the Analysis of Beam Dump Experiments: Production of an axion, a dark photon, or a new axial-vector boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Gerald A. Miller, Yu-Sheng Liu","submitted_at":"2017-05-03T21:27:39Z","abstract_excerpt":"Beam dump experiments have been used to search for new particles, $\\phi$, with null results interpreted in terms of limits on masses $m_\\phi$ and coupling constants $\\epsilon$. However these limits have been obtained by using approximations [including the Weizs\\\"{a}cker-Williams (WW) approximation] or Monte-Carlo simulations. We display methods to obtain the cross section and the resulting particle production rates without using approximations on the phase space integral or Monte-Carlo simulations. In our previous work we examined the case of the new scalar boson production; in this paper we e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01633","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":"1705.01633","created_at":"2026-05-18T00:40:03.778919+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.01633v1","created_at":"2026-05-18T00:40:03.778919+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01633","created_at":"2026-05-18T00:40:03.778919+00:00"},{"alias_kind":"pith_short_12","alias_value":"YPYVKXUUTLWK","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"YPYVKXUUTLWK55MM","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"YPYVKXUU","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2503.15630","citing_title":"Supernova production of axion-like particles coupling to electrons, reloaded","ref_index":78,"is_internal_anchor":true},{"citing_arxiv_id":"2510.25613","citing_title":"Muon Beam Dump Experiments explicate five-dimensional nature of $U(1)_{L_{\\mu}-L_{\\tau}}$","ref_index":81,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM","json":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM.json","graph_json":"https://pith.science/api/pith-number/YPYVKXUUTLWK55MM6KFNS4KDKM/graph.json","events_json":"https://pith.science/api/pith-number/YPYVKXUUTLWK55MM6KFNS4KDKM/events.json","paper":"https://pith.science/paper/YPYVKXUU"},"agent_actions":{"view_html":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM","download_json":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM.json","view_paper":"https://pith.science/paper/YPYVKXUU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.01633&json=true","fetch_graph":"https://pith.science/api/pith-number/YPYVKXUUTLWK55MM6KFNS4KDKM/graph.json","fetch_events":"https://pith.science/api/pith-number/YPYVKXUUTLWK55MM6KFNS4KDKM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM/action/storage_attestation","attest_author":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM/action/author_attestation","sign_citation":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM/action/citation_signature","submit_replication":"https://pith.science/pith/YPYVKXUUTLWK55MM6KFNS4KDKM/action/replication_record"}},"created_at":"2026-05-18T00:40:03.778919+00:00","updated_at":"2026-05-18T00:40:03.778919+00:00"}