{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:XKPDQV7ZVIMFQAT6PCG2MCBM5T","short_pith_number":"pith:XKPDQV7Z","schema_version":"1.0","canonical_sha256":"ba9e3857f9aa1858027e788da6082cecca92be96fc99b0c8b3f35f1fbe45b554","source":{"kind":"arxiv","id":"1401.6505","version":3},"attestation_state":"computed","paper":{"title":"Holographic entanglement entropy in insulator/superconductor transition with Born-Infeld electrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Jiliang Jing, Weiping Yao","submitted_at":"2014-01-25T08:36:09Z","abstract_excerpt":"We investigate the holographic entanglement entropy in the insulator/superconductor phase transition for the Born-Infeld electrodynamics with full backreaction in five-dimensional AdS soliton spacetime. We note that the holographic entanglement entropy is a good probe to study the properties of the phase transition, and the Born-Infeld factor $b$ has no effect on the critical chemical potential $\\mu_c$. We find that both in the half space and the belt one, the non-monotonic behavior of the entanglement entropy versus the chemical potential is a general property, and the entanglement entropy in"},"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":"1401.6505","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-01-25T08:36:09Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"f82170ba30af7d9a5707a7d16bb513aea780fc0fad3f5cb52b3af6f9fd66b081","abstract_canon_sha256":"0241ea00538cf84d59dba6bd003bb8f7bb3b6c78c1520c33bc5fb41fb18b8d3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:16.946337Z","signature_b64":"iJeguF9i04MM6zoD+GZe8xbX2VMNfCVqPVDkwY40a8VrnR6Cstw1UxImB32TP8Gyc2NMyccSOcsdWx7lwfGACQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba9e3857f9aa1858027e788da6082cecca92be96fc99b0c8b3f35f1fbe45b554","last_reissued_at":"2026-05-18T01:45:16.945823Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:16.945823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic entanglement entropy in insulator/superconductor transition with Born-Infeld electrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Jiliang Jing, Weiping Yao","submitted_at":"2014-01-25T08:36:09Z","abstract_excerpt":"We investigate the holographic entanglement entropy in the insulator/superconductor phase transition for the Born-Infeld electrodynamics with full backreaction in five-dimensional AdS soliton spacetime. We note that the holographic entanglement entropy is a good probe to study the properties of the phase transition, and the Born-Infeld factor $b$ has no effect on the critical chemical potential $\\mu_c$. We find that both in the half space and the belt one, the non-monotonic behavior of the entanglement entropy versus the chemical potential is a general property, and the entanglement entropy in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.6505","kind":"arxiv","version":3},"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":"1401.6505","created_at":"2026-05-18T01:45:16.945922+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.6505v3","created_at":"2026-05-18T01:45:16.945922+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.6505","created_at":"2026-05-18T01:45:16.945922+00:00"},{"alias_kind":"pith_short_12","alias_value":"XKPDQV7ZVIMF","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"XKPDQV7ZVIMFQAT6","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"XKPDQV7Z","created_at":"2026-05-18T12:28:57.508820+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/XKPDQV7ZVIMFQAT6PCG2MCBM5T","json":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T.json","graph_json":"https://pith.science/api/pith-number/XKPDQV7ZVIMFQAT6PCG2MCBM5T/graph.json","events_json":"https://pith.science/api/pith-number/XKPDQV7ZVIMFQAT6PCG2MCBM5T/events.json","paper":"https://pith.science/paper/XKPDQV7Z"},"agent_actions":{"view_html":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T","download_json":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T.json","view_paper":"https://pith.science/paper/XKPDQV7Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.6505&json=true","fetch_graph":"https://pith.science/api/pith-number/XKPDQV7ZVIMFQAT6PCG2MCBM5T/graph.json","fetch_events":"https://pith.science/api/pith-number/XKPDQV7ZVIMFQAT6PCG2MCBM5T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T/action/storage_attestation","attest_author":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T/action/author_attestation","sign_citation":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T/action/citation_signature","submit_replication":"https://pith.science/pith/XKPDQV7ZVIMFQAT6PCG2MCBM5T/action/replication_record"}},"created_at":"2026-05-18T01:45:16.945922+00:00","updated_at":"2026-05-18T01:45:16.945922+00:00"}