{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:7QZQDKIFD4GEDRLDZUMMFVDMUA","short_pith_number":"pith:7QZQDKIF","schema_version":"1.0","canonical_sha256":"fc3301a9051f0c41c563cd18c2d46ca01908c5434f092cf044fdaa134c054439","source":{"kind":"arxiv","id":"0904.2523","version":1},"attestation_state":"computed","paper":{"title":"Structure of the flux lines lattice in NbSe2: Equilibrium state and influence of the magnetic history","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Brulet, A. Pautrat, C.D. Dewhurst, Ch. Simon, M. Aburas, M.J. Higgins, P. Mathieu, S. Bhattacharya","submitted_at":"2009-04-16T15:32:44Z","abstract_excerpt":"We have performed small-angle neutron scattering (SANS) of the flux line lattice (FLL) in a Fe doped NbSe_2 sample which presents a large peak effect in the critical current. The scattered intensity and the width of the Bragg peaks of the equilibrium FLL indicate an ordered structure in the peak effect zone. The history dependence in the FLL structure has been studied using field cooled and zero field cooled procedures, and each state shows the same intensity of Bragg scattering and good orientational order. These results strongly suggest that the peak effect is unrelated to a bulk disordering"},"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":"0904.2523","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2009-04-16T15:32:44Z","cross_cats_sorted":[],"title_canon_sha256":"2262cfff160b604245e585ba6fa2693a0872c932d20fe1d3eebc4c8ce5d77aa3","abstract_canon_sha256":"c4faf4226d0fa82ad7763796e16ec026bbfff0f1adbe83ceae7791dd7af53765"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:13:59.829792Z","signature_b64":"Z0iaUX8XVJuWf50p8PWfOzX7iXIuF0YxgorkGox5UFndUle7dBMiCyMnO+2XeXtgIJt0fLTPeH4ZRhHcxl0NAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc3301a9051f0c41c563cd18c2d46ca01908c5434f092cf044fdaa134c054439","last_reissued_at":"2026-05-18T02:13:59.829053Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:13:59.829053Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Structure of the flux lines lattice in NbSe2: Equilibrium state and influence of the magnetic history","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Brulet, A. Pautrat, C.D. Dewhurst, Ch. Simon, M. Aburas, M.J. Higgins, P. Mathieu, S. Bhattacharya","submitted_at":"2009-04-16T15:32:44Z","abstract_excerpt":"We have performed small-angle neutron scattering (SANS) of the flux line lattice (FLL) in a Fe doped NbSe_2 sample which presents a large peak effect in the critical current. The scattered intensity and the width of the Bragg peaks of the equilibrium FLL indicate an ordered structure in the peak effect zone. The history dependence in the FLL structure has been studied using field cooled and zero field cooled procedures, and each state shows the same intensity of Bragg scattering and good orientational order. These results strongly suggest that the peak effect is unrelated to a bulk disordering"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.2523","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":"0904.2523","created_at":"2026-05-18T02:13:59.829175+00:00"},{"alias_kind":"arxiv_version","alias_value":"0904.2523v1","created_at":"2026-05-18T02:13:59.829175+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.2523","created_at":"2026-05-18T02:13:59.829175+00:00"},{"alias_kind":"pith_short_12","alias_value":"7QZQDKIFD4GE","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_16","alias_value":"7QZQDKIFD4GEDRLD","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_8","alias_value":"7QZQDKIF","created_at":"2026-05-18T12:25:58.837520+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/7QZQDKIFD4GEDRLDZUMMFVDMUA","json":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA.json","graph_json":"https://pith.science/api/pith-number/7QZQDKIFD4GEDRLDZUMMFVDMUA/graph.json","events_json":"https://pith.science/api/pith-number/7QZQDKIFD4GEDRLDZUMMFVDMUA/events.json","paper":"https://pith.science/paper/7QZQDKIF"},"agent_actions":{"view_html":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA","download_json":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA.json","view_paper":"https://pith.science/paper/7QZQDKIF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0904.2523&json=true","fetch_graph":"https://pith.science/api/pith-number/7QZQDKIFD4GEDRLDZUMMFVDMUA/graph.json","fetch_events":"https://pith.science/api/pith-number/7QZQDKIFD4GEDRLDZUMMFVDMUA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA/action/storage_attestation","attest_author":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA/action/author_attestation","sign_citation":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA/action/citation_signature","submit_replication":"https://pith.science/pith/7QZQDKIFD4GEDRLDZUMMFVDMUA/action/replication_record"}},"created_at":"2026-05-18T02:13:59.829175+00:00","updated_at":"2026-05-18T02:13:59.829175+00:00"}