{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:5JPKCQU7LBJ3NM3RADOCLQ5UXX","short_pith_number":"pith:5JPKCQU7","schema_version":"1.0","canonical_sha256":"ea5ea1429f5853b6b37100dc25c3b4bdd0069cda63c97646767ceb92a7aea55f","source":{"kind":"arxiv","id":"nucl-th/9905026","version":1},"attestation_state":"computed","paper":{"title":"Compton Scattering by Nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A.I. L'vov (Moscow), A.I. Milstein (Novosibirsk), M. Schumacher (Goettingen), M.-Th. Huett (Goettingen)","submitted_at":"1999-05-13T16:14:02Z","abstract_excerpt":"The concept of Compton scattering by even-even nuclei from giant-resonance to nucleon-resonance energies and the status of experimental and theoretical researches in this field are outlined. Nuclear Compton scattering in the giant-resonance energy-region provides information on the dynamical properties of the in-medium mass of the nucleon. The electromagnetic polarizabilities of the nucleon in the nuclear medium can be extracted from nuclear Compton scattering data obtained in the quasi-deuteron energy-region. Recent results are presented for two-body effects due to the mesonic seagull amplitu"},"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":"nucl-th/9905026","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-13T16:14:02Z","cross_cats_sorted":[],"title_canon_sha256":"f69c7858606866e82df201a06e7107b8501f7a1b21bb3e562e97f805667843b7","abstract_canon_sha256":"3d6abc1a34a6a60fe0f996a79c87509edb8a5525449c23c33d38180586fa9269"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:31.502736Z","signature_b64":"AXSfaEoYK8ngNAMu4p1P4IS/oBqJugkLPFIwx2Lxlz62BJSoqRIT+kfDkwY67zJmcB24K9wL71E+KjdPTEvaDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea5ea1429f5853b6b37100dc25c3b4bdd0069cda63c97646767ceb92a7aea55f","last_reissued_at":"2026-05-18T02:35:31.502280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:31.502280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Compton Scattering by Nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A.I. L'vov (Moscow), A.I. Milstein (Novosibirsk), M. Schumacher (Goettingen), M.-Th. Huett (Goettingen)","submitted_at":"1999-05-13T16:14:02Z","abstract_excerpt":"The concept of Compton scattering by even-even nuclei from giant-resonance to nucleon-resonance energies and the status of experimental and theoretical researches in this field are outlined. Nuclear Compton scattering in the giant-resonance energy-region provides information on the dynamical properties of the in-medium mass of the nucleon. The electromagnetic polarizabilities of the nucleon in the nuclear medium can be extracted from nuclear Compton scattering data obtained in the quasi-deuteron energy-region. Recent results are presented for two-body effects due to the mesonic seagull amplitu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9905026","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":"nucl-th/9905026","created_at":"2026-05-18T02:35:31.502358+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9905026v1","created_at":"2026-05-18T02:35:31.502358+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9905026","created_at":"2026-05-18T02:35:31.502358+00:00"},{"alias_kind":"pith_short_12","alias_value":"5JPKCQU7LBJ3","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_16","alias_value":"5JPKCQU7LBJ3NM3R","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_8","alias_value":"5JPKCQU7","created_at":"2026-05-18T12:25:49.038998+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.05449","citing_title":"Manifest Gauge Invariance for Structure Dependent Radiative Corrections to Processes Involving Atoms and Nuclei","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX","json":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX.json","graph_json":"https://pith.science/api/pith-number/5JPKCQU7LBJ3NM3RADOCLQ5UXX/graph.json","events_json":"https://pith.science/api/pith-number/5JPKCQU7LBJ3NM3RADOCLQ5UXX/events.json","paper":"https://pith.science/paper/5JPKCQU7"},"agent_actions":{"view_html":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX","download_json":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX.json","view_paper":"https://pith.science/paper/5JPKCQU7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9905026&json=true","fetch_graph":"https://pith.science/api/pith-number/5JPKCQU7LBJ3NM3RADOCLQ5UXX/graph.json","fetch_events":"https://pith.science/api/pith-number/5JPKCQU7LBJ3NM3RADOCLQ5UXX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX/action/storage_attestation","attest_author":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX/action/author_attestation","sign_citation":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX/action/citation_signature","submit_replication":"https://pith.science/pith/5JPKCQU7LBJ3NM3RADOCLQ5UXX/action/replication_record"}},"created_at":"2026-05-18T02:35:31.502358+00:00","updated_at":"2026-05-18T02:35:31.502358+00:00"}