{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:XFGFYNYOHGOKT7346KCBUJD5IV","short_pith_number":"pith:XFGFYNYO","canonical_record":{"source":{"id":"1512.06661","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-30T17:29:03Z","cross_cats_sorted":[],"title_canon_sha256":"76086cb1936472812bf6058860d9e4cbdc94c2b9e3901b2485df4e77e3af0d1c","abstract_canon_sha256":"2f0df090c794f2d11352d9ec67ce26e4e5d78ae5a9c265e7809da5c8a27ca317"},"schema_version":"1.0"},"canonical_sha256":"b94c5c370e399ca9ff7cf2841a247d454b350004e22aadaa90f4da85ce78c553","source":{"kind":"arxiv","id":"1512.06661","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.06661","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"arxiv_version","alias_value":"1512.06661v1","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.06661","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"pith_short_12","alias_value":"XFGFYNYOHGOK","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"XFGFYNYOHGOKT734","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"XFGFYNYO","created_at":"2026-05-18T12:29:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:XFGFYNYOHGOKT7346KCBUJD5IV","target":"record","payload":{"canonical_record":{"source":{"id":"1512.06661","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-30T17:29:03Z","cross_cats_sorted":[],"title_canon_sha256":"76086cb1936472812bf6058860d9e4cbdc94c2b9e3901b2485df4e77e3af0d1c","abstract_canon_sha256":"2f0df090c794f2d11352d9ec67ce26e4e5d78ae5a9c265e7809da5c8a27ca317"},"schema_version":"1.0"},"canonical_sha256":"b94c5c370e399ca9ff7cf2841a247d454b350004e22aadaa90f4da85ce78c553","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:02:04.651340Z","signature_b64":"HEWlTPu91bMkwTVWQQLtt8NB8uZgPzX+MNp4bpkHINGryVktaAj7omcVZ2gdTbxabclzowMar03sBofCzZi0Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b94c5c370e399ca9ff7cf2841a247d454b350004e22aadaa90f4da85ce78c553","last_reissued_at":"2026-05-18T01:02:04.650711Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:02:04.650711Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.06661","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:02:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mJFPX3xqqkmUSuC88y8toOmZGBXxD3NwZTjDPAtmkExOdlvG1bE3IJftJDPW45jHNXs2k3rbIvF8LZwOU6JIDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:30:38.525761Z"},"content_sha256":"a1e9a361768dc20b5e1e36586931a755532d8a429cc2c4943d4a0c0c2380e5dd","schema_version":"1.0","event_id":"sha256:a1e9a361768dc20b5e1e36586931a755532d8a429cc2c4943d4a0c0c2380e5dd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:XFGFYNYOHGOKT7346KCBUJD5IV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-equilibrium phase and entanglement entropy in 2D holographic superconductors via Gauge-String duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. Momeni, H. Gholizade, M. Raza, N.S. Mazhari, R. Myrzakulov","submitted_at":"2015-10-30T17:29:03Z","abstract_excerpt":"An alternative method of developing the theory of non-equilibrium two dimensional holographic superconductor is to start from the definition of a time dependent $AdS_3$ background. As originally proposed, many of these formulae were cast in exponential form, but the adoption of the numeric method of expression throughout the bulk serves to show more clearly the relationship between the various parameters. The time dependence behaviour of the scalar condensation and Maxwell fields are fitted numerically. A usual value for Maxwell field on AdS horizon is $\\exp(-bt)$, and the exponential $\\log$ r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.06661","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:02:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"34Zm3CerkmgM7AomW89Bi39zsl0IB3LARauYWO+JdNYBpKEvfNvVX4SUbHeUVPsNImqXHDQSb9GtQEz/rs0NDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T16:30:38.526309Z"},"content_sha256":"c7f2d0c75775f585b247005e51bf3829c256b3a2f4905d0bc6f7745768f1f7af","schema_version":"1.0","event_id":"sha256:c7f2d0c75775f585b247005e51bf3829c256b3a2f4905d0bc6f7745768f1f7af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XFGFYNYOHGOKT7346KCBUJD5IV/bundle.json","state_url":"https://pith.science/pith/XFGFYNYOHGOKT7346KCBUJD5IV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XFGFYNYOHGOKT7346KCBUJD5IV/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":"2026-05-31T16:30:38Z","links":{"resolver":"https://pith.science/pith/XFGFYNYOHGOKT7346KCBUJD5IV","bundle":"https://pith.science/pith/XFGFYNYOHGOKT7346KCBUJD5IV/bundle.json","state":"https://pith.science/pith/XFGFYNYOHGOKT7346KCBUJD5IV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XFGFYNYOHGOKT7346KCBUJD5IV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:XFGFYNYOHGOKT7346KCBUJD5IV","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":"2f0df090c794f2d11352d9ec67ce26e4e5d78ae5a9c265e7809da5c8a27ca317","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-30T17:29:03Z","title_canon_sha256":"76086cb1936472812bf6058860d9e4cbdc94c2b9e3901b2485df4e77e3af0d1c"},"schema_version":"1.0","source":{"id":"1512.06661","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.06661","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"arxiv_version","alias_value":"1512.06661v1","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.06661","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"pith_short_12","alias_value":"XFGFYNYOHGOK","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"XFGFYNYOHGOKT734","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"XFGFYNYO","created_at":"2026-05-18T12:29:50Z"}],"graph_snapshots":[{"event_id":"sha256:c7f2d0c75775f585b247005e51bf3829c256b3a2f4905d0bc6f7745768f1f7af","target":"graph","created_at":"2026-05-18T01:02:04Z","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":"An alternative method of developing the theory of non-equilibrium two dimensional holographic superconductor is to start from the definition of a time dependent $AdS_3$ background. As originally proposed, many of these formulae were cast in exponential form, but the adoption of the numeric method of expression throughout the bulk serves to show more clearly the relationship between the various parameters. The time dependence behaviour of the scalar condensation and Maxwell fields are fitted numerically. A usual value for Maxwell field on AdS horizon is $\\exp(-bt)$, and the exponential $\\log$ r","authors_text":"D. Momeni, H. Gholizade, M. Raza, N.S. Mazhari, R. Myrzakulov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-30T17:29:03Z","title":"Non-equilibrium phase and entanglement entropy in 2D holographic superconductors via Gauge-String duality"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.06661","kind":"arxiv","version":1},"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:a1e9a361768dc20b5e1e36586931a755532d8a429cc2c4943d4a0c0c2380e5dd","target":"record","created_at":"2026-05-18T01:02:04Z","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":"2f0df090c794f2d11352d9ec67ce26e4e5d78ae5a9c265e7809da5c8a27ca317","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-30T17:29:03Z","title_canon_sha256":"76086cb1936472812bf6058860d9e4cbdc94c2b9e3901b2485df4e77e3af0d1c"},"schema_version":"1.0","source":{"id":"1512.06661","kind":"arxiv","version":1}},"canonical_sha256":"b94c5c370e399ca9ff7cf2841a247d454b350004e22aadaa90f4da85ce78c553","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b94c5c370e399ca9ff7cf2841a247d454b350004e22aadaa90f4da85ce78c553","first_computed_at":"2026-05-18T01:02:04.650711Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:04.650711Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HEWlTPu91bMkwTVWQQLtt8NB8uZgPzX+MNp4bpkHINGryVktaAj7omcVZ2gdTbxabclzowMar03sBofCzZi0Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:04.651340Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.06661","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1e9a361768dc20b5e1e36586931a755532d8a429cc2c4943d4a0c0c2380e5dd","sha256:c7f2d0c75775f585b247005e51bf3829c256b3a2f4905d0bc6f7745768f1f7af"],"state_sha256":"584c1bf066c7dc8e3b1a97889198162121e569ef240fa362e8d79481f51bc49d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PjFAMhzh7H3jq+stLX1mrVhM9gH7KV4Xk0tUHO4H2aIXB96TxPmMCn6PM3N8bTkY8fiVl5sMUSglaz7mjX6WBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T16:30:38.529960Z","bundle_sha256":"50022dfd19cb216a786500e99c4ba5606b9b7145773b062d2eab2ec2b180e120"}}