{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:GIFBKQTXHQGG7GVKKK7ZJ4S3I3","short_pith_number":"pith:GIFBKQTX","schema_version":"1.0","canonical_sha256":"320a1542773c0c6f9aaa52bf94f25b46c5007c7656fe1d305ca4e4d891c6dd9b","source":{"kind":"arxiv","id":"1602.01122","version":1},"attestation_state":"computed","paper":{"title":"Size-induced depression of first-order transition lines and entropy-jump in extremely-layered nanocrystalline vortex matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"H. Pastoriza, M.I. Dolz, M. Konczykowski, M. Li, N. R. Cejas Bolecek, V. Mosser, Y. Fasano","submitted_at":"2016-02-02T21:31:36Z","abstract_excerpt":"We detect the persistence of the solidification and order-disorder first-order transition lines in the phase diagram of nanocrystalline Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8}$ vortex matter down to a system size of less than hundred vortices. The temperature-location of the vortex solidification transition line is not altered by decreasing the sample size although there is a depletion of the entropy-jump at the transition with respect to macroscopic vortex matter. The solid order-disorder phase transition field moves upward on decreasing the system size due to the increase of the surface-to-volume r"},"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":"1602.01122","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-02-02T21:31:36Z","cross_cats_sorted":[],"title_canon_sha256":"545b85ba005196470b8b45c205cd5d682742fbf0f112c56339e2ffccadf0baa4","abstract_canon_sha256":"a512f4b4a06bca89877a6e7fb1fe68edac160ee77471fceea0f33e5c21e41ecc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:23.543911Z","signature_b64":"Ao+Qs1YNicvkKMNZwmm7uSAWyjYJ9ff3llUqD5+pAX6qlhEJzGU9rsu3Az3vTw5vJqE+HXOv21oE4ihHhgUHBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"320a1542773c0c6f9aaa52bf94f25b46c5007c7656fe1d305ca4e4d891c6dd9b","last_reissued_at":"2026-05-18T01:21:23.543331Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:23.543331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Size-induced depression of first-order transition lines and entropy-jump in extremely-layered nanocrystalline vortex matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"H. Pastoriza, M.I. Dolz, M. Konczykowski, M. Li, N. R. Cejas Bolecek, V. Mosser, Y. Fasano","submitted_at":"2016-02-02T21:31:36Z","abstract_excerpt":"We detect the persistence of the solidification and order-disorder first-order transition lines in the phase diagram of nanocrystalline Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8}$ vortex matter down to a system size of less than hundred vortices. The temperature-location of the vortex solidification transition line is not altered by decreasing the sample size although there is a depletion of the entropy-jump at the transition with respect to macroscopic vortex matter. The solid order-disorder phase transition field moves upward on decreasing the system size due to the increase of the surface-to-volume r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.01122","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":"1602.01122","created_at":"2026-05-18T01:21:23.543425+00:00"},{"alias_kind":"arxiv_version","alias_value":"1602.01122v1","created_at":"2026-05-18T01:21:23.543425+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.01122","created_at":"2026-05-18T01:21:23.543425+00:00"},{"alias_kind":"pith_short_12","alias_value":"GIFBKQTXHQGG","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_16","alias_value":"GIFBKQTXHQGG7GVK","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_8","alias_value":"GIFBKQTX","created_at":"2026-05-18T12:30:19.053100+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/GIFBKQTXHQGG7GVKKK7ZJ4S3I3","json":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3.json","graph_json":"https://pith.science/api/pith-number/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/graph.json","events_json":"https://pith.science/api/pith-number/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/events.json","paper":"https://pith.science/paper/GIFBKQTX"},"agent_actions":{"view_html":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3","download_json":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3.json","view_paper":"https://pith.science/paper/GIFBKQTX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1602.01122&json=true","fetch_graph":"https://pith.science/api/pith-number/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/graph.json","fetch_events":"https://pith.science/api/pith-number/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/action/storage_attestation","attest_author":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/action/author_attestation","sign_citation":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/action/citation_signature","submit_replication":"https://pith.science/pith/GIFBKQTXHQGG7GVKKK7ZJ4S3I3/action/replication_record"}},"created_at":"2026-05-18T01:21:23.543425+00:00","updated_at":"2026-05-18T01:21:23.543425+00:00"}