{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:7SWPFTN24KKLORJMONEKPTCIJD","short_pith_number":"pith:7SWPFTN2","schema_version":"1.0","canonical_sha256":"fcacf2cdbae294b7452c7348a7cc4848eb812bf7f087add5ae45df1bde5539bc","source":{"kind":"arxiv","id":"1202.3816","version":1},"attestation_state":"computed","paper":{"title":"Shielding experiments by the JASMIN collaboration at Fermilab (II) - Radioactivity measurement induced by secondary particles from the anti-proton production target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Anthony Leveling, David Boehnlein, Gary Lauten, Hiroshi Iwase (KEK, Hiroshi Matsumura, Hiroshi Nakashima, Hiroshi Yashima (Kyoto U., Ibaraki), Kamran Vaziri (Fermilab), Koji Oishi (Shimizu, KURRI), Nikolai Mokhov, Norihiro Matsuda, Norikazu Kinoshita (KEK, Tokyo), Tsukuba), Tsukuba & Tsukuba U.), Yoshimi Kasugai (JAEA, Yukio Sakamoto (JAEA","submitted_at":"2012-02-16T23:05:41Z","abstract_excerpt":"The JASMIN Collaboration has performed an experiment to conduct measurements of nuclear reaction rates around the anti-proton production (Pbar) target at the Fermi National Accelerator Laboratory (FNAL). At the Pbar target station, the target, consisting an Inconel 600 cylinder, was irradiated by a 120 GeV/c proton beam from the FNAL Main Injector. The beam intensity was 3.6 x 10**12 protons per second. Samples of Al, Nb, Cu, and Au were placed near the target to investigate the spatial and energy distribution of secondary particles emitted from it. After irradiation, the induced activities of"},"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":"1202.3816","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2012-02-16T23:05:41Z","cross_cats_sorted":[],"title_canon_sha256":"a191fecaf934c535f867a69564223d974a72bf18c01731e775b489488f34ad3b","abstract_canon_sha256":"ab8703fceadf6818c2737690b23e7e663539c6b218a332fff5837e2137b2144a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:02:02.691622Z","signature_b64":"clWJXSgvtMQcpAinMsRjV5r2QcpPmkjltiCK2MwWS3/ru358IP/8dm70wWwy7ojS3ePh+EiL0YIzMr/2p84QDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fcacf2cdbae294b7452c7348a7cc4848eb812bf7f087add5ae45df1bde5539bc","last_reissued_at":"2026-05-18T04:02:02.691041Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:02:02.691041Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shielding experiments by the JASMIN collaboration at Fermilab (II) - Radioactivity measurement induced by secondary particles from the anti-proton production target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Anthony Leveling, David Boehnlein, Gary Lauten, Hiroshi Iwase (KEK, Hiroshi Matsumura, Hiroshi Nakashima, Hiroshi Yashima (Kyoto U., Ibaraki), Kamran Vaziri (Fermilab), Koji Oishi (Shimizu, KURRI), Nikolai Mokhov, Norihiro Matsuda, Norikazu Kinoshita (KEK, Tokyo), Tsukuba), Tsukuba & Tsukuba U.), Yoshimi Kasugai (JAEA, Yukio Sakamoto (JAEA","submitted_at":"2012-02-16T23:05:41Z","abstract_excerpt":"The JASMIN Collaboration has performed an experiment to conduct measurements of nuclear reaction rates around the anti-proton production (Pbar) target at the Fermi National Accelerator Laboratory (FNAL). At the Pbar target station, the target, consisting an Inconel 600 cylinder, was irradiated by a 120 GeV/c proton beam from the FNAL Main Injector. The beam intensity was 3.6 x 10**12 protons per second. Samples of Al, Nb, Cu, and Au were placed near the target to investigate the spatial and energy distribution of secondary particles emitted from it. After irradiation, the induced activities of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.3816","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":"1202.3816","created_at":"2026-05-18T04:02:02.691136+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.3816v1","created_at":"2026-05-18T04:02:02.691136+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.3816","created_at":"2026-05-18T04:02:02.691136+00:00"},{"alias_kind":"pith_short_12","alias_value":"7SWPFTN24KKL","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_16","alias_value":"7SWPFTN24KKLORJM","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_8","alias_value":"7SWPFTN2","created_at":"2026-05-18T12:26:58.693483+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/7SWPFTN24KKLORJMONEKPTCIJD","json":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD.json","graph_json":"https://pith.science/api/pith-number/7SWPFTN24KKLORJMONEKPTCIJD/graph.json","events_json":"https://pith.science/api/pith-number/7SWPFTN24KKLORJMONEKPTCIJD/events.json","paper":"https://pith.science/paper/7SWPFTN2"},"agent_actions":{"view_html":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD","download_json":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD.json","view_paper":"https://pith.science/paper/7SWPFTN2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.3816&json=true","fetch_graph":"https://pith.science/api/pith-number/7SWPFTN24KKLORJMONEKPTCIJD/graph.json","fetch_events":"https://pith.science/api/pith-number/7SWPFTN24KKLORJMONEKPTCIJD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD/action/storage_attestation","attest_author":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD/action/author_attestation","sign_citation":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD/action/citation_signature","submit_replication":"https://pith.science/pith/7SWPFTN24KKLORJMONEKPTCIJD/action/replication_record"}},"created_at":"2026-05-18T04:02:02.691136+00:00","updated_at":"2026-05-18T04:02:02.691136+00:00"}