{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:TM72OLR35TLERFZFZWXNPAFLPN","short_pith_number":"pith:TM72OLR3","canonical_record":{"source":{"id":"2604.13104","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-10T15:42:19Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"cc4266d6c2373f0c09b085e9f965e83e562b245c9d0b5882b9efe82273ccd0e5","abstract_canon_sha256":"645926e0fd6739defd72b6b3ebc15fba0d8c830be693205793c93638310b13ca"},"schema_version":"1.0"},"canonical_sha256":"9b3fa72e3becd6489725cdaed780ab7b5b13702ec59a44f76f902f64d66e124f","source":{"kind":"arxiv","id":"2604.13104","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.13104","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"arxiv_version","alias_value":"2604.13104v2","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.13104","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_12","alias_value":"TM72OLR35TLE","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_16","alias_value":"TM72OLR35TLERFZF","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_8","alias_value":"TM72OLR3","created_at":"2026-08-03T01:15:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:TM72OLR35TLERFZFZWXNPAFLPN","target":"record","payload":{"canonical_record":{"source":{"id":"2604.13104","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-10T15:42:19Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"cc4266d6c2373f0c09b085e9f965e83e562b245c9d0b5882b9efe82273ccd0e5","abstract_canon_sha256":"645926e0fd6739defd72b6b3ebc15fba0d8c830be693205793c93638310b13ca"},"schema_version":"1.0"},"canonical_sha256":"9b3fa72e3becd6489725cdaed780ab7b5b13702ec59a44f76f902f64d66e124f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-03T01:15:00.535686Z","signature_b64":"wGgUfy4HoQobyD4M4/ivx1JEqG2EnwjNIYowluJ69qpdFh47BoJSZITiyE9vi9p+nmNejBeiErYULuqocKz8AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b3fa72e3becd6489725cdaed780ab7b5b13702ec59a44f76f902f64d66e124f","last_reissued_at":"2026-08-03T01:15:00.533934Z","signature_status":"signed_v1","first_computed_at":"2026-08-03T01:15:00.533934Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2604.13104","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":"2026-08-03T01:15:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wZtrrfVKhDHQmAiRGQ4V1hwKpEDdxZ347DwOB17cJ/b3ktisXDgq4q9UnC+0B4FLtpoXIoqCC7ORUBwJdw+pAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T18:47:32.955123Z"},"content_sha256":"90bc8450126466c96ae710e3cd59331ba1dbcb024ab80c5a812846880fd07c50","schema_version":"1.0","event_id":"sha256:90bc8450126466c96ae710e3cd59331ba1dbcb024ab80c5a812846880fd07c50"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:TM72OLR35TLERFZFZWXNPAFLPN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonequilibrium crossover in the supercritical region from quench dynamics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region.","cross_cats":["hep-ph","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Jing-Fei Zhang, Xin Zhang, Zhang-Yu Nie, Zi-Qiang Zhao","submitted_at":"2026-04-10T15:42:19Z","abstract_excerpt":"Distinguishing different subphases in the supercritical region is an important issue in statistical physics and condensed matter physics. Traditional approaches rely mainly on static thermodynamic response functions or equilibrium correlation functions, which are essentially limited to quasistatic processes. In this paper, we investigate the evolution behavior of a system after a rapid quench from the perspective of nonequilibrium dynamics within a holographic model. We find that, using the time at which inhomogeneous structures appear most rapidly, we can define a supercritical crossover curv"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"the invasion phenomenon induced by topological defects persists in the supercritical region, and the invasion velocity exhibits a clear turning point as a function of the quench endpoint ρ_f. This turning point defines a new nonequilibrium supercritical crossover line.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the observed turning point in invasion velocity corresponds to a physically meaningful crossover line rather than a numerical or model-specific feature, and that the holographic superfluid model faithfully represents the relevant real-world dynamics.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Quench dynamics in a holographic superfluid reveal a nonequilibrium crossover line in the supercritical region defined by a turning point in invasion velocity.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"c2e286df10666b165d362972b9b74e8c30d676c1a88be67a6fcfa09a4c3d867f"},"source":{"id":"2604.13104","kind":"arxiv","version":2},"verdict":{"id":"8066b7c8-d86b-464a-ab78-dbaf422b6396","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-10T17:08:11.360303Z","strongest_claim":"the invasion phenomenon induced by topological defects persists in the supercritical region, and the invasion velocity exhibits a clear turning point as a function of the quench endpoint ρ_f. This turning point defines a new nonequilibrium supercritical crossover line.","one_line_summary":"Quench dynamics in a holographic superfluid reveal a nonequilibrium crossover line in the supercritical region defined by a turning point in invasion velocity.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the observed turning point in invasion velocity corresponds to a physically meaningful crossover line rather than a numerical or model-specific feature, and that the holographic superfluid model faithfully represents the relevant real-world dynamics.","pith_extraction_headline":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2604.13104/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"8066b7c8-d86b-464a-ab78-dbaf422b6396"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-03T01:15:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2qycTurIR15gRX+M3CEg5PEjR76xfvQI8aZS5QW9XnrmyasDEdcsVINPjqgFcL8Tir03bZHpEYs4/z678CoWBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T18:47:32.955610Z"},"content_sha256":"d0a966880642454b60ec62bcccf9ef9b1f012a1a1b9131919c35af7231d93a8f","schema_version":"1.0","event_id":"sha256:d0a966880642454b60ec62bcccf9ef9b1f012a1a1b9131919c35af7231d93a8f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TM72OLR35TLERFZFZWXNPAFLPN/bundle.json","state_url":"https://pith.science/pith/TM72OLR35TLERFZFZWXNPAFLPN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TM72OLR35TLERFZFZWXNPAFLPN/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":"2026-08-04T18:47:32Z","links":{"resolver":"https://pith.science/pith/TM72OLR35TLERFZFZWXNPAFLPN","bundle":"https://pith.science/pith/TM72OLR35TLERFZFZWXNPAFLPN/bundle.json","state":"https://pith.science/pith/TM72OLR35TLERFZFZWXNPAFLPN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TM72OLR35TLERFZFZWXNPAFLPN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:TM72OLR35TLERFZFZWXNPAFLPN","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":"645926e0fd6739defd72b6b3ebc15fba0d8c830be693205793c93638310b13ca","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-10T15:42:19Z","title_canon_sha256":"cc4266d6c2373f0c09b085e9f965e83e562b245c9d0b5882b9efe82273ccd0e5"},"schema_version":"1.0","source":{"id":"2604.13104","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.13104","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"arxiv_version","alias_value":"2604.13104v2","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.13104","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_12","alias_value":"TM72OLR35TLE","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_16","alias_value":"TM72OLR35TLERFZF","created_at":"2026-08-03T01:15:00Z"},{"alias_kind":"pith_short_8","alias_value":"TM72OLR3","created_at":"2026-08-03T01:15:00Z"}],"graph_snapshots":[{"event_id":"sha256:d0a966880642454b60ec62bcccf9ef9b1f012a1a1b9131919c35af7231d93a8f","target":"graph","created_at":"2026-08-03T01:15:00Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"the invasion phenomenon induced by topological defects persists in the supercritical region, and the invasion velocity exhibits a clear turning point as a function of the quench endpoint ρ_f. This turning point defines a new nonequilibrium supercritical crossover line."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the observed turning point in invasion velocity corresponds to a physically meaningful crossover line rather than a numerical or model-specific feature, and that the holographic superfluid model faithfully represents the relevant real-world dynamics."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Quench dynamics in a holographic superfluid reveal a nonequilibrium crossover line in the supercritical region defined by a turning point in invasion velocity."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region."}],"snapshot_sha256":"c2e286df10666b165d362972b9b74e8c30d676c1a88be67a6fcfa09a4c3d867f"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2604.13104/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Distinguishing different subphases in the supercritical region is an important issue in statistical physics and condensed matter physics. Traditional approaches rely mainly on static thermodynamic response functions or equilibrium correlation functions, which are essentially limited to quasistatic processes. In this paper, we investigate the evolution behavior of a system after a rapid quench from the perspective of nonequilibrium dynamics within a holographic model. We find that, using the time at which inhomogeneous structures appear most rapidly, we can define a supercritical crossover curv","authors_text":"Jing-Fei Zhang, Xin Zhang, Zhang-Yu Nie, Zi-Qiang Zhao","cross_cats":["hep-ph","hep-th"],"headline":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-10T15:42:19Z","title":"Nonequilibrium crossover in the supercritical region from quench dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2604.13104","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-10T17:08:11.360303Z","id":"8066b7c8-d86b-464a-ab78-dbaf422b6396","model_set":{"reader":"grok-4.3"},"one_line_summary":"Quench dynamics in a holographic superfluid reveal a nonequilibrium crossover line in the supercritical region defined by a turning point in invasion velocity.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Invasion velocity of topological defects turns at a specific point, defining a new nonequilibrium crossover line in the supercritical region.","strongest_claim":"the invasion phenomenon induced by topological defects persists in the supercritical region, and the invasion velocity exhibits a clear turning point as a function of the quench endpoint ρ_f. This turning point defines a new nonequilibrium supercritical crossover line.","weakest_assumption":"That the observed turning point in invasion velocity corresponds to a physically meaningful crossover line rather than a numerical or model-specific feature, and that the holographic superfluid model faithfully represents the relevant real-world dynamics."}},"verdict_id":"8066b7c8-d86b-464a-ab78-dbaf422b6396"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:90bc8450126466c96ae710e3cd59331ba1dbcb024ab80c5a812846880fd07c50","target":"record","created_at":"2026-08-03T01:15:00Z","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":"645926e0fd6739defd72b6b3ebc15fba0d8c830be693205793c93638310b13ca","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-10T15:42:19Z","title_canon_sha256":"cc4266d6c2373f0c09b085e9f965e83e562b245c9d0b5882b9efe82273ccd0e5"},"schema_version":"1.0","source":{"id":"2604.13104","kind":"arxiv","version":2}},"canonical_sha256":"9b3fa72e3becd6489725cdaed780ab7b5b13702ec59a44f76f902f64d66e124f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9b3fa72e3becd6489725cdaed780ab7b5b13702ec59a44f76f902f64d66e124f","first_computed_at":"2026-08-03T01:15:00.533934Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-03T01:15:00.533934Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wGgUfy4HoQobyD4M4/ivx1JEqG2EnwjNIYowluJ69qpdFh47BoJSZITiyE9vi9p+nmNejBeiErYULuqocKz8AA==","signature_status":"signed_v1","signed_at":"2026-08-03T01:15:00.535686Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.13104","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:90bc8450126466c96ae710e3cd59331ba1dbcb024ab80c5a812846880fd07c50","sha256:d0a966880642454b60ec62bcccf9ef9b1f012a1a1b9131919c35af7231d93a8f"],"state_sha256":"72e87d406bc01288903bd4586f7651498284881d7517a56a725d2c3ed83cf1eb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uoN2AMUi9zoMv6wa4jHUv9rjueZaDecyl1Vig6USHVcCKrlUUNvv6U5YfKeR0ZlEgnqfmNcYhyvsJPh2DVScCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T18:47:32.958492Z","bundle_sha256":"ea859be40f5f547bbbbf0eaae86f0e87abf355df9e2fbbe60e60756219165b16"}}