{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:M25EQT4CXHMCUNGXVHVTPKHO2G","short_pith_number":"pith:M25EQT4C","canonical_record":{"source":{"id":"1412.3878","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-12T03:39:50Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4d5cb986a0d6c222f9c913aaf818409c9b3e1bef231d9f55a4609880e43c6231","abstract_canon_sha256":"1287a2bc7aca36a77778a60f59a1272abdd823e87fe8d171239f0b123efc8b01"},"schema_version":"1.0"},"canonical_sha256":"66ba484f82b9d82a34d7a9eb37a8eed18e69fc6264669ac2cfeaa697ae9fc73d","source":{"kind":"arxiv","id":"1412.3878","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.3878","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"arxiv_version","alias_value":"1412.3878v2","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3878","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"pith_short_12","alias_value":"M25EQT4CXHMC","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"M25EQT4CXHMCUNGX","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"M25EQT4C","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:M25EQT4CXHMCUNGXVHVTPKHO2G","target":"record","payload":{"canonical_record":{"source":{"id":"1412.3878","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-12T03:39:50Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4d5cb986a0d6c222f9c913aaf818409c9b3e1bef231d9f55a4609880e43c6231","abstract_canon_sha256":"1287a2bc7aca36a77778a60f59a1272abdd823e87fe8d171239f0b123efc8b01"},"schema_version":"1.0"},"canonical_sha256":"66ba484f82b9d82a34d7a9eb37a8eed18e69fc6264669ac2cfeaa697ae9fc73d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:38.495537Z","signature_b64":"USBv7f+zgLVavr/UDzUpFkW9A9/ZA+lMKrsHU/MdgQqxqdkeB7dcnRLox42jqEqFFNfBsAYfyubszE65K2hyAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66ba484f82b9d82a34d7a9eb37a8eed18e69fc6264669ac2cfeaa697ae9fc73d","last_reissued_at":"2026-05-18T02:26:38.494962Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:38.494962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.3878","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:26:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LjXK6dl9HXXUAnViB9s1sfe7HvInwgDzuSIYFRpaP8WLJKivtms2mIO8dVk5oY6X9J7nh3/Yp+eldi5RdTU1Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T06:46:05.878922Z"},"content_sha256":"f3be7b814ec7166a19d804e50cb3d616744ba61570632639686a6180d1f84967","schema_version":"1.0","event_id":"sha256:f3be7b814ec7166a19d804e50cb3d616744ba61570632639686a6180d1f84967"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:M25EQT4CXHMCUNGXVHVTPKHO2G","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic thermalization with a chemical potential from Born-Infeld electrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Bertha Cuadros-Melgar, Elcio Abdalla, Giancarlo Camilo","submitted_at":"2014-12-12T03:39:50Z","abstract_excerpt":"The problem of holographic thermalization in the framework of Einstein gravity coupled to Born-Infeld nonlinear electrodynamics is investigated. We use equal time two-point correlation functions and expectation values of Wilson loop operators in the boundary quantum field theory as probes of thermalization, which have dual gravity descriptions in terms of geodesic lengths and minimal area surfaces in the bulk spacetime. The full range of values of the chemical potential per temperature ratio on the boundary is explored. The numerical results show that the effect of the charge on the thermaliza"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3878","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:26:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jBkdHyQdp2CmsCEPQDjYvBveU28KM71aGEPn1fVrbA5dBOa7CHBZa2HTJ5/DsiNOypksW9G4qhVooaLNCBHODg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T06:46:05.879280Z"},"content_sha256":"01b44b34a5e9ca889b6c372c9d3e592b406f878aa6a95a9f9108d2df30327645","schema_version":"1.0","event_id":"sha256:01b44b34a5e9ca889b6c372c9d3e592b406f878aa6a95a9f9108d2df30327645"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/bundle.json","state_url":"https://pith.science/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-01T06:46:05Z","links":{"resolver":"https://pith.science/pith/M25EQT4CXHMCUNGXVHVTPKHO2G","bundle":"https://pith.science/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/bundle.json","state":"https://pith.science/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M25EQT4CXHMCUNGXVHVTPKHO2G/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:M25EQT4CXHMCUNGXVHVTPKHO2G","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"1287a2bc7aca36a77778a60f59a1272abdd823e87fe8d171239f0b123efc8b01","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-12T03:39:50Z","title_canon_sha256":"4d5cb986a0d6c222f9c913aaf818409c9b3e1bef231d9f55a4609880e43c6231"},"schema_version":"1.0","source":{"id":"1412.3878","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.3878","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"arxiv_version","alias_value":"1412.3878v2","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3878","created_at":"2026-05-18T02:26:38Z"},{"alias_kind":"pith_short_12","alias_value":"M25EQT4CXHMC","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"M25EQT4CXHMCUNGX","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"M25EQT4C","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:01b44b34a5e9ca889b6c372c9d3e592b406f878aa6a95a9f9108d2df30327645","target":"graph","created_at":"2026-05-18T02:26:38Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The problem of holographic thermalization in the framework of Einstein gravity coupled to Born-Infeld nonlinear electrodynamics is investigated. We use equal time two-point correlation functions and expectation values of Wilson loop operators in the boundary quantum field theory as probes of thermalization, which have dual gravity descriptions in terms of geodesic lengths and minimal area surfaces in the bulk spacetime. The full range of values of the chemical potential per temperature ratio on the boundary is explored. The numerical results show that the effect of the charge on the thermaliza","authors_text":"Bertha Cuadros-Melgar, Elcio Abdalla, Giancarlo Camilo","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-12T03:39:50Z","title":"Holographic thermalization with a chemical potential from Born-Infeld electrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3878","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:f3be7b814ec7166a19d804e50cb3d616744ba61570632639686a6180d1f84967","target":"record","created_at":"2026-05-18T02:26:38Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"1287a2bc7aca36a77778a60f59a1272abdd823e87fe8d171239f0b123efc8b01","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-12T03:39:50Z","title_canon_sha256":"4d5cb986a0d6c222f9c913aaf818409c9b3e1bef231d9f55a4609880e43c6231"},"schema_version":"1.0","source":{"id":"1412.3878","kind":"arxiv","version":2}},"canonical_sha256":"66ba484f82b9d82a34d7a9eb37a8eed18e69fc6264669ac2cfeaa697ae9fc73d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"66ba484f82b9d82a34d7a9eb37a8eed18e69fc6264669ac2cfeaa697ae9fc73d","first_computed_at":"2026-05-18T02:26:38.494962Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:26:38.494962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"USBv7f+zgLVavr/UDzUpFkW9A9/ZA+lMKrsHU/MdgQqxqdkeB7dcnRLox42jqEqFFNfBsAYfyubszE65K2hyAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:26:38.495537Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.3878","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f3be7b814ec7166a19d804e50cb3d616744ba61570632639686a6180d1f84967","sha256:01b44b34a5e9ca889b6c372c9d3e592b406f878aa6a95a9f9108d2df30327645"],"state_sha256":"83e0ddeb22bc4fd2028c9d0fc6f309d6321aa65165cc001488b072bde0faec35"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O20/JPWlNWcyIUDlicTUsdOU1fYxB6qS+UzjJ/q3d+tLgSNZgrgIB8EA8sE3MVV2VjQ4WpBekna4Lrn+OfdkAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-01T06:46:05.881607Z","bundle_sha256":"5ca8deb467d5f8375be61a6e284582d53daaea9ace2477b1171da2e631149aa7"}}