{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:Q2FP2JLJ54T7S6MTCJJBVUJ77C","short_pith_number":"pith:Q2FP2JLJ","schema_version":"1.0","canonical_sha256":"868afd2569ef27f9799312521ad13ff8bbe15c2fd38ab2c05373122de5a0b33b","source":{"kind":"arxiv","id":"1403.1584","version":1},"attestation_state":"computed","paper":{"title":"Time-reversal invariance violation measurement using polarized neutron scattering from polarized xenon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Pinghan Chu","submitted_at":"2014-03-06T21:00:58Z","abstract_excerpt":"We proposed to use polarized neutrons scattering from a hyperpolarized 131Xe gaseous target in order to measure time-reversal violation effect in baryon processes with nucleons. This article provides a brief introduction, historical review, and possible methods to construct a hyperpolarized 131Xe gaseous target."},"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":"1403.1584","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2014-03-06T21:00:58Z","cross_cats_sorted":[],"title_canon_sha256":"b51434b5529642c896c3a820f88dfd076e7fd4f04db601055880c929960a7a0b","abstract_canon_sha256":"1aba5b9c45f24ffa292b8aa71187df59af118cdb8dc0b908fe039365d236d3b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:53.029237Z","signature_b64":"BcyaYYs6HvSPy2UuFx8T8jxspzTY4lDsXYkhk0VGsXbJg91+n8eAH4DHq1M9VPuEsWYrAW1jhJWX+9vqPbLMAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"868afd2569ef27f9799312521ad13ff8bbe15c2fd38ab2c05373122de5a0b33b","last_reissued_at":"2026-05-18T02:56:53.028839Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:53.028839Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Time-reversal invariance violation measurement using polarized neutron scattering from polarized xenon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"Pinghan Chu","submitted_at":"2014-03-06T21:00:58Z","abstract_excerpt":"We proposed to use polarized neutrons scattering from a hyperpolarized 131Xe gaseous target in order to measure time-reversal violation effect in baryon processes with nucleons. This article provides a brief introduction, historical review, and possible methods to construct a hyperpolarized 131Xe gaseous target."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.1584","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":"1403.1584","created_at":"2026-05-18T02:56:53.028896+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.1584v1","created_at":"2026-05-18T02:56:53.028896+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.1584","created_at":"2026-05-18T02:56:53.028896+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q2FP2JLJ54T7","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q2FP2JLJ54T7S6MT","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q2FP2JLJ","created_at":"2026-05-18T12:28:43.426989+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/Q2FP2JLJ54T7S6MTCJJBVUJ77C","json":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C.json","graph_json":"https://pith.science/api/pith-number/Q2FP2JLJ54T7S6MTCJJBVUJ77C/graph.json","events_json":"https://pith.science/api/pith-number/Q2FP2JLJ54T7S6MTCJJBVUJ77C/events.json","paper":"https://pith.science/paper/Q2FP2JLJ"},"agent_actions":{"view_html":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C","download_json":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C.json","view_paper":"https://pith.science/paper/Q2FP2JLJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.1584&json=true","fetch_graph":"https://pith.science/api/pith-number/Q2FP2JLJ54T7S6MTCJJBVUJ77C/graph.json","fetch_events":"https://pith.science/api/pith-number/Q2FP2JLJ54T7S6MTCJJBVUJ77C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C/action/storage_attestation","attest_author":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C/action/author_attestation","sign_citation":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C/action/citation_signature","submit_replication":"https://pith.science/pith/Q2FP2JLJ54T7S6MTCJJBVUJ77C/action/replication_record"}},"created_at":"2026-05-18T02:56:53.028896+00:00","updated_at":"2026-05-18T02:56:53.028896+00:00"}