{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:R2BLSYZV7KTKE3JC7GCJGE5X6B","short_pith_number":"pith:R2BLSYZV","schema_version":"1.0","canonical_sha256":"8e82b96335faa6a26d22f9849313b7f04aef27f48ded4a42bc629c512b62bd1c","source":{"kind":"arxiv","id":"2209.14712","version":1},"attestation_state":"computed","paper":{"title":"A method for computing hadron-nucleus cross sections in fully active sampling calorimetric targets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"David W. Schmitz, Johnny Ho","submitted_at":"2022-09-26T21:40:50Z","abstract_excerpt":"Interaction cross section measurements in fixed-target scattering experiments are typically performed by measuring the attenuation of a beam of particles that is incident upon a target slab of material. A fully active sampling calorimeter, such as the time projection chamber, is a more voluminous target that can be treated as a series of smaller target slabs. We present a method of computing hadron-nucleus interaction cross sections for data taken with fully active sampling calorimeters that is robust even if the target is comprised of numerous slabs of various thicknesses."},"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":"2209.14712","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2022-09-26T21:40:50Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"8642a18d00161a8cd0859fe5284718572e91a5cce0f2cac2aaa09347384b51ec","abstract_canon_sha256":"ce59d737f19541e6ccba073501fe05f189d7ece91d0d650c2ec4ada36103a9c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:02:04.927750Z","signature_b64":"7QwcI6Sw1o5fn6M73I8b6q8pFgbQ3yb1K7RenSWAs2EPEvpvYYeRaAcAUncWNAbr+D0g3sHPzju/vJC5WPQtBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e82b96335faa6a26d22f9849313b7f04aef27f48ded4a42bc629c512b62bd1c","last_reissued_at":"2026-07-05T05:02:04.927351Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:02:04.927351Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A method for computing hadron-nucleus cross sections in fully active sampling calorimetric targets","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"David W. Schmitz, Johnny Ho","submitted_at":"2022-09-26T21:40:50Z","abstract_excerpt":"Interaction cross section measurements in fixed-target scattering experiments are typically performed by measuring the attenuation of a beam of particles that is incident upon a target slab of material. A fully active sampling calorimeter, such as the time projection chamber, is a more voluminous target that can be treated as a series of smaller target slabs. We present a method of computing hadron-nucleus interaction cross sections for data taken with fully active sampling calorimeters that is robust even if the target is comprised of numerous slabs of various thicknesses."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.14712","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.14712/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2209.14712","created_at":"2026-07-05T05:02:04.927409+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.14712v1","created_at":"2026-07-05T05:02:04.927409+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.14712","created_at":"2026-07-05T05:02:04.927409+00:00"},{"alias_kind":"pith_short_12","alias_value":"R2BLSYZV7KTK","created_at":"2026-07-05T05:02:04.927409+00:00"},{"alias_kind":"pith_short_16","alias_value":"R2BLSYZV7KTKE3JC","created_at":"2026-07-05T05:02:04.927409+00:00"},{"alias_kind":"pith_short_8","alias_value":"R2BLSYZV","created_at":"2026-07-05T05:02:04.927409+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/R2BLSYZV7KTKE3JC7GCJGE5X6B","json":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B.json","graph_json":"https://pith.science/api/pith-number/R2BLSYZV7KTKE3JC7GCJGE5X6B/graph.json","events_json":"https://pith.science/api/pith-number/R2BLSYZV7KTKE3JC7GCJGE5X6B/events.json","paper":"https://pith.science/paper/R2BLSYZV"},"agent_actions":{"view_html":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B","download_json":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B.json","view_paper":"https://pith.science/paper/R2BLSYZV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.14712&json=true","fetch_graph":"https://pith.science/api/pith-number/R2BLSYZV7KTKE3JC7GCJGE5X6B/graph.json","fetch_events":"https://pith.science/api/pith-number/R2BLSYZV7KTKE3JC7GCJGE5X6B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B/action/storage_attestation","attest_author":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B/action/author_attestation","sign_citation":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B/action/citation_signature","submit_replication":"https://pith.science/pith/R2BLSYZV7KTKE3JC7GCJGE5X6B/action/replication_record"}},"created_at":"2026-07-05T05:02:04.927409+00:00","updated_at":"2026-07-05T05:02:04.927409+00:00"}