{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:S2HE2YBPBHNQCTJWP5NYLU72UT","short_pith_number":"pith:S2HE2YBP","schema_version":"1.0","canonical_sha256":"968e4d602f09db014d367f5b85d3faa4f8c9abf440d254b1fcec70ff476e5d54","source":{"kind":"arxiv","id":"0903.2389","version":1},"attestation_state":"computed","paper":{"title":"Real-space vortex glass imaging and the vortex phase diagram of SnMo6S8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A.B. Antunes, A. Demuer, A. Par\\'e, A.P. Petrovic, C. Senatore, D. Salloum, M. Potel, {\\O}. Fischer, P. Gougeon, R. Lortz, Y. Fasano","submitted_at":"2009-03-13T13:47:05Z","abstract_excerpt":"Using scanning tunnelling microscopy at 400mK, we have obtained maps of around 100 vortices in SnMo6S8 from 2 - 9T. The orientational and positional disorder at 5 and 9T show that these are the first large-scale images of a vortex glass. At higher temperature a magnetisation peak effect is observed, whose upper boundary coincides with a lambda anomaly in the specific heat. Our data favour a kinetic glass description of the vortex melting transition, indicating that vortex topological disorder persists at fields and temperatures far below the peak effect in low-Tc superconductors."},"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":"0903.2389","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2009-03-13T13:47:05Z","cross_cats_sorted":[],"title_canon_sha256":"269013adb6855e6690a318a62ddb7d749749afc26c75afe14b933ccc1709fd62","abstract_canon_sha256":"49bcf6f55fccc38acefa1dd2df94f0d8ac3a19cbb69271da25214696a3b3d97b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:54.692713Z","signature_b64":"4C7LI/Qfk0Vi+X/Mv9uuAQ3z2QdA1uIceXR0cORcJoW02y/SRg0JXGZV6fEY961Lh+wn1foGTZG8sy81lEvrBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"968e4d602f09db014d367f5b85d3faa4f8c9abf440d254b1fcec70ff476e5d54","last_reissued_at":"2026-05-18T03:31:54.692118Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:54.692118Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Real-space vortex glass imaging and the vortex phase diagram of SnMo6S8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A.B. Antunes, A. Demuer, A. Par\\'e, A.P. Petrovic, C. Senatore, D. Salloum, M. Potel, {\\O}. Fischer, P. Gougeon, R. Lortz, Y. Fasano","submitted_at":"2009-03-13T13:47:05Z","abstract_excerpt":"Using scanning tunnelling microscopy at 400mK, we have obtained maps of around 100 vortices in SnMo6S8 from 2 - 9T. The orientational and positional disorder at 5 and 9T show that these are the first large-scale images of a vortex glass. At higher temperature a magnetisation peak effect is observed, whose upper boundary coincides with a lambda anomaly in the specific heat. Our data favour a kinetic glass description of the vortex melting transition, indicating that vortex topological disorder persists at fields and temperatures far below the peak effect in low-Tc superconductors."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.2389","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":"0903.2389","created_at":"2026-05-18T03:31:54.692191+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.2389v1","created_at":"2026-05-18T03:31:54.692191+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.2389","created_at":"2026-05-18T03:31:54.692191+00:00"},{"alias_kind":"pith_short_12","alias_value":"S2HE2YBPBHNQ","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"S2HE2YBPBHNQCTJW","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"S2HE2YBP","created_at":"2026-05-18T12:26:01.383474+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/S2HE2YBPBHNQCTJWP5NYLU72UT","json":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT.json","graph_json":"https://pith.science/api/pith-number/S2HE2YBPBHNQCTJWP5NYLU72UT/graph.json","events_json":"https://pith.science/api/pith-number/S2HE2YBPBHNQCTJWP5NYLU72UT/events.json","paper":"https://pith.science/paper/S2HE2YBP"},"agent_actions":{"view_html":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT","download_json":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT.json","view_paper":"https://pith.science/paper/S2HE2YBP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.2389&json=true","fetch_graph":"https://pith.science/api/pith-number/S2HE2YBPBHNQCTJWP5NYLU72UT/graph.json","fetch_events":"https://pith.science/api/pith-number/S2HE2YBPBHNQCTJWP5NYLU72UT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT/action/storage_attestation","attest_author":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT/action/author_attestation","sign_citation":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT/action/citation_signature","submit_replication":"https://pith.science/pith/S2HE2YBPBHNQCTJWP5NYLU72UT/action/replication_record"}},"created_at":"2026-05-18T03:31:54.692191+00:00","updated_at":"2026-05-18T03:31:54.692191+00:00"}