{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:YZLDUV6ZDUUMKXMS7SUDOJ2ABM","short_pith_number":"pith:YZLDUV6Z","schema_version":"1.0","canonical_sha256":"c6563a57d91d28c55d92fca83727400b3920ba09d951f82ecbaee4a83db0a72c","source":{"kind":"arxiv","id":"1601.01249","version":4},"attestation_state":"computed","paper":{"title":"Simulations of background sources in AMoRE-I experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Luqman, D.H. Ha, E.J. Jeon, H.J. Kim, H.K. Park, H.S. Jo, H.S. Lee, J.H. So, J.J. Lee, K. Siyeon, V.I. Tretyak, V.V. Kobychev, Y.D. Kim, Y.H. Kim, Y.S. Yoon","submitted_at":"2016-01-06T17:57:19Z","abstract_excerpt":"The first phase of the Advanced Mo-based Rare Process Experiment (AMoRE-I), an experimental search for neutrinoless double beta decay (0$\\nu\\beta\\beta$) of $^{100}$Mo in calcium molybdate (CMO) crystal using cryogenic techniques, is in preparation at the YangYang underground laboratory (Y2L) in South Korea. A GEANT4 based Monte Carlo simulation was performed for background estimation in the first-phase the AMoRE-I detector and shield configuration. Background sources such as $^{238}$U, $^{232}$Th, $^{40}$K, $^{235}$U, and $^{210}$Pb were simulated from inside the crystals, surrounding material"},"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":"1601.01249","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-01-06T17:57:19Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e2e0b4efb3f8ff33cdd47111720be27e9e28bc1816388b1212d4f4d4cf20e61d","abstract_canon_sha256":"9f62285ab7d0f1db824cf2ecdd6446a07c0e637b48e180a12cd04c1bd9d0508a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:42.964429Z","signature_b64":"MmEKUg8bbIvgZuvdTXcXIOQShlAb+4CUJEeQEQMLbMo+8dzvQfjvIQaMAgdgDZy+cWkr8YqkyvLOlyi8+UAYCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6563a57d91d28c55d92fca83727400b3920ba09d951f82ecbaee4a83db0a72c","last_reissued_at":"2026-05-18T00:46:42.963834Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:42.963834Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulations of background sources in AMoRE-I experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Luqman, D.H. Ha, E.J. Jeon, H.J. Kim, H.K. Park, H.S. Jo, H.S. Lee, J.H. So, J.J. Lee, K. Siyeon, V.I. Tretyak, V.V. Kobychev, Y.D. Kim, Y.H. Kim, Y.S. Yoon","submitted_at":"2016-01-06T17:57:19Z","abstract_excerpt":"The first phase of the Advanced Mo-based Rare Process Experiment (AMoRE-I), an experimental search for neutrinoless double beta decay (0$\\nu\\beta\\beta$) of $^{100}$Mo in calcium molybdate (CMO) crystal using cryogenic techniques, is in preparation at the YangYang underground laboratory (Y2L) in South Korea. A GEANT4 based Monte Carlo simulation was performed for background estimation in the first-phase the AMoRE-I detector and shield configuration. Background sources such as $^{238}$U, $^{232}$Th, $^{40}$K, $^{235}$U, and $^{210}$Pb were simulated from inside the crystals, surrounding material"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01249","kind":"arxiv","version":4},"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":"1601.01249","created_at":"2026-05-18T00:46:42.963908+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.01249v4","created_at":"2026-05-18T00:46:42.963908+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01249","created_at":"2026-05-18T00:46:42.963908+00:00"},{"alias_kind":"pith_short_12","alias_value":"YZLDUV6ZDUUM","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"YZLDUV6ZDUUMKXMS","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"YZLDUV6Z","created_at":"2026-05-18T12:30:53.716459+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/YZLDUV6ZDUUMKXMS7SUDOJ2ABM","json":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM.json","graph_json":"https://pith.science/api/pith-number/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/graph.json","events_json":"https://pith.science/api/pith-number/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/events.json","paper":"https://pith.science/paper/YZLDUV6Z"},"agent_actions":{"view_html":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM","download_json":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM.json","view_paper":"https://pith.science/paper/YZLDUV6Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.01249&json=true","fetch_graph":"https://pith.science/api/pith-number/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/graph.json","fetch_events":"https://pith.science/api/pith-number/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/action/storage_attestation","attest_author":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/action/author_attestation","sign_citation":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/action/citation_signature","submit_replication":"https://pith.science/pith/YZLDUV6ZDUUMKXMS7SUDOJ2ABM/action/replication_record"}},"created_at":"2026-05-18T00:46:42.963908+00:00","updated_at":"2026-05-18T00:46:42.963908+00:00"}