{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:7ZNYN36BN5ZPWPBUMMBIIPOZ6V","short_pith_number":"pith:7ZNYN36B","schema_version":"1.0","canonical_sha256":"fe5b86efc16f72fb3c346302843dd9f57c937b184e073366a056c2b29cd2afdd","source":{"kind":"arxiv","id":"1001.2142","version":1},"attestation_state":"computed","paper":{"title":"Observations of Pauli Paramagnetic Effects on the Flux Line Lattice in CeCoIn5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A.D. Bianchi, C. Petrovic, E.D. Bauer, E.M. Forgan, J.L. Gavilano, J.L. Sarrao, J. Mesot, J.S. White, L. DeBeer-Schmitt, M. Kenzelmann, M.R. Eskildsen, M. Zolliker, P. Das, R. Movshovich, S. Gerber","submitted_at":"2010-01-13T12:55:32Z","abstract_excerpt":"From small-angle neutron scattering studies of the flux line lattice (FLL) in CeCoIn5, with magnetic field applied parallel to the crystal c-axis, we obtain the field- and temperature-dependence of the FLL form factor, which is a measure of the spatial variation of the field in the mixed state. We extend our earlier work [A.D. Bianchi et al. 2008 Science 319, 177] to temperatures up to 1250 mK. Over the entire temperature range, paramagnetism in the flux line cores results in an increase of the form factor with field. Near H_c2 the form factor decreases again, and our results indicate that thi"},"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":"1001.2142","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-01-13T12:55:32Z","cross_cats_sorted":[],"title_canon_sha256":"55b100c67723f3b14ad0f22ce0b47c06324a72765c2882147b0a3adb5aae8173","abstract_canon_sha256":"7216d18fc314d98de9161c80d68d9d50cba76c5a7485ccad776dcbbebf35a79a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:22:03.933479Z","signature_b64":"/PLQVgrK5x64iM+Ern2IUO/JPfwwX5r2K1FTMExUukMNTy3yRPqge9PwMQVgX4SZpDMockFVwEujZKvJ3UshAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe5b86efc16f72fb3c346302843dd9f57c937b184e073366a056c2b29cd2afdd","last_reissued_at":"2026-07-04T17:22:03.933042Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:22:03.933042Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Observations of Pauli Paramagnetic Effects on the Flux Line Lattice in CeCoIn5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A.D. Bianchi, C. Petrovic, E.D. Bauer, E.M. Forgan, J.L. Gavilano, J.L. Sarrao, J. Mesot, J.S. White, L. DeBeer-Schmitt, M. Kenzelmann, M.R. Eskildsen, M. Zolliker, P. Das, R. Movshovich, S. Gerber","submitted_at":"2010-01-13T12:55:32Z","abstract_excerpt":"From small-angle neutron scattering studies of the flux line lattice (FLL) in CeCoIn5, with magnetic field applied parallel to the crystal c-axis, we obtain the field- and temperature-dependence of the FLL form factor, which is a measure of the spatial variation of the field in the mixed state. We extend our earlier work [A.D. Bianchi et al. 2008 Science 319, 177] to temperatures up to 1250 mK. Over the entire temperature range, paramagnetism in the flux line cores results in an increase of the form factor with field. Near H_c2 the form factor decreases again, and our results indicate that thi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.2142","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/1001.2142/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":"1001.2142","created_at":"2026-07-04T17:22:03.933109+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.2142v1","created_at":"2026-07-04T17:22:03.933109+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.2142","created_at":"2026-07-04T17:22:03.933109+00:00"},{"alias_kind":"pith_short_12","alias_value":"7ZNYN36BN5ZP","created_at":"2026-07-04T17:22:03.933109+00:00"},{"alias_kind":"pith_short_16","alias_value":"7ZNYN36BN5ZPWPBU","created_at":"2026-07-04T17:22:03.933109+00:00"},{"alias_kind":"pith_short_8","alias_value":"7ZNYN36B","created_at":"2026-07-04T17:22:03.933109+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/7ZNYN36BN5ZPWPBUMMBIIPOZ6V","json":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V.json","graph_json":"https://pith.science/api/pith-number/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/graph.json","events_json":"https://pith.science/api/pith-number/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/events.json","paper":"https://pith.science/paper/7ZNYN36B"},"agent_actions":{"view_html":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V","download_json":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V.json","view_paper":"https://pith.science/paper/7ZNYN36B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.2142&json=true","fetch_graph":"https://pith.science/api/pith-number/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/graph.json","fetch_events":"https://pith.science/api/pith-number/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/action/storage_attestation","attest_author":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/action/author_attestation","sign_citation":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/action/citation_signature","submit_replication":"https://pith.science/pith/7ZNYN36BN5ZPWPBUMMBIIPOZ6V/action/replication_record"}},"created_at":"2026-07-04T17:22:03.933109+00:00","updated_at":"2026-07-04T17:22:03.933109+00:00"}