{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:U6FD2V6BVWGXX5LMDSHFGN5DIF","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":"9e48ee548c56ae13ffa3b76237fe371a351b6fb86a2e06f1868239fac0f2d2c9","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-19T12:53:58Z","title_canon_sha256":"a59128cb814b2dd85459734894884304318b91173244d739d6afcec1d71d59c3"},"schema_version":"1.0","source":{"id":"2205.09532","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.09532","created_at":"2026-07-05T05:04:29Z"},{"alias_kind":"arxiv_version","alias_value":"2205.09532v3","created_at":"2026-07-05T05:04:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.09532","created_at":"2026-07-05T05:04:29Z"},{"alias_kind":"pith_short_12","alias_value":"U6FD2V6BVWGX","created_at":"2026-07-05T05:04:29Z"},{"alias_kind":"pith_short_16","alias_value":"U6FD2V6BVWGXX5LM","created_at":"2026-07-05T05:04:29Z"},{"alias_kind":"pith_short_8","alias_value":"U6FD2V6B","created_at":"2026-07-05T05:04:29Z"}],"graph_snapshots":[{"event_id":"sha256:353d7c2b3ac7d3d332fb6901a5cbba5698230bdbbc8e4fb6bd854ce3c3ab45e7","target":"graph","created_at":"2026-07-05T05:04:29Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2205.09532/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper, we consider the time evolution of charge imbalance resolved negativity after a global quench in the 1+1 dimensional complex Klein-Gordon theory. We focus on two types of global quenches which are called boundary state quench and mass quench respectively. We first study the boundary state quench where the post-quench dynamic is governed by a massless Hamiltonian. In this case, the temporal evolution of charged imbalance resolved negativity can be obtained first by evaluating the correlators of the fluxed twist field in the upper half plane and then applying Fourier transformation","authors_text":"Hui-Huang Chen","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-19T12:53:58Z","title":"Dynamics of charge imbalance resolved negativity after a global quench in free scalar field theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.09532","kind":"arxiv","version":3},"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":"sha256:4775717440a8cd60470e8daf3b576c7659cdfeb84f60e1165931bb03b60cd207","target":"record","created_at":"2026-07-05T05:04:29Z","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":"9e48ee548c56ae13ffa3b76237fe371a351b6fb86a2e06f1868239fac0f2d2c9","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-19T12:53:58Z","title_canon_sha256":"a59128cb814b2dd85459734894884304318b91173244d739d6afcec1d71d59c3"},"schema_version":"1.0","source":{"id":"2205.09532","kind":"arxiv","version":3}},"canonical_sha256":"a78a3d57c1ad8d7bf56c1c8e5337a3417d39740cc2770339e843558bb9a4dd0d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a78a3d57c1ad8d7bf56c1c8e5337a3417d39740cc2770339e843558bb9a4dd0d","first_computed_at":"2026-07-05T05:04:29.224292Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:04:29.224292Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AlM8baHdq3S0ZlAzvjYTajV/InwQJEhDJu5sJeyyeqbKQvaDBkz0CwmIj04I4fhRUI52WuSMIKYlIHjC5UpdAw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:04:29.224767Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.09532","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4775717440a8cd60470e8daf3b576c7659cdfeb84f60e1165931bb03b60cd207","sha256:353d7c2b3ac7d3d332fb6901a5cbba5698230bdbbc8e4fb6bd854ce3c3ab45e7"],"state_sha256":"2c29fa9bc93bb0ba0a8d17e548a713de44a488353742b108649d4461f61aa6e0"}