{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:PVM6SSWCTDHTHSXPQNDAVKNZHZ","short_pith_number":"pith:PVM6SSWC","canonical_record":{"source":{"id":"2506.16308","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-19T13:29:51Z","cross_cats_sorted":["cond-mat.quant-gas","physics.optics","quant-ph"],"title_canon_sha256":"e91c09592e43214b5d3fe5124587625b3798b59b49362d20230554a4513aff36","abstract_canon_sha256":"0a80df50beed5a04a4808b4a559602cdfabc9f82bcb3ba55daf542b8d62ceec6"},"schema_version":"1.0"},"canonical_sha256":"7d59e94ac298cf33caef83460aa9b93e59bc1836e81237cdb4f7dc4fb7500d9c","source":{"kind":"arxiv","id":"2506.16308","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.16308","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"arxiv_version","alias_value":"2506.16308v2","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.16308","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_12","alias_value":"PVM6SSWCTDHT","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_16","alias_value":"PVM6SSWCTDHTHSXP","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_8","alias_value":"PVM6SSWC","created_at":"2026-06-23T01:11:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:PVM6SSWCTDHTHSXPQNDAVKNZHZ","target":"record","payload":{"canonical_record":{"source":{"id":"2506.16308","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-19T13:29:51Z","cross_cats_sorted":["cond-mat.quant-gas","physics.optics","quant-ph"],"title_canon_sha256":"e91c09592e43214b5d3fe5124587625b3798b59b49362d20230554a4513aff36","abstract_canon_sha256":"0a80df50beed5a04a4808b4a559602cdfabc9f82bcb3ba55daf542b8d62ceec6"},"schema_version":"1.0"},"canonical_sha256":"7d59e94ac298cf33caef83460aa9b93e59bc1836e81237cdb4f7dc4fb7500d9c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-23T01:11:55.888574Z","signature_b64":"5mqznSyjBCOd/koCh6cVBTcH5aeyGUOnb9pLbD8f8pLyz86RvlrU8BHTIQpPE69PbexLXNKGNVgVbnchmlFgBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d59e94ac298cf33caef83460aa9b93e59bc1836e81237cdb4f7dc4fb7500d9c","last_reissued_at":"2026-06-23T01:11:55.888071Z","signature_status":"signed_v1","first_computed_at":"2026-06-23T01:11:55.888071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2506.16308","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":"2026-06-23T01:11:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7RY35T8mP9WdP3gWrJ3uWGIILi+QGKka90E4URzEgLHc1HWrMbC8ogpyQJcA1lGQb29I9Om2vmfytCFFCRkwAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T12:02:19.792782Z"},"content_sha256":"afd8cf4b25721bba2ee6c9299b6820b831f22564eda02bdf84217bec1fd60b67","schema_version":"1.0","event_id":"sha256:afd8cf4b25721bba2ee6c9299b6820b831f22564eda02bdf84217bec1fd60b67"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:PVM6SSWCTDHTHSXPQNDAVKNZHZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum dynamical signatures of non-Hermitian boundary modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Emil J. Bergholtz, Fan Yang, Maria Zelenayova, Paolo Molignini","submitted_at":"2025-06-19T13:29:51Z","abstract_excerpt":"The non-Hermitian bulk-boundary correspondence features an interplay between the non-Hermitian skin effect and anomalous boundary-mode behavior. Whereas the skin effect is known to manifest itself in quantum dynamics in the form of chiral damping, it has remained less clear what impact the boundary modes may have. Here we derive experimentally accessible signatures of the boundary modes. We also establish clear criteria, based on the generalized Brillouin zone, that determine when bulk and boundary effects can be dynamically discerned using the Liouvillian separation gap. This leads to telltal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.16308","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2506.16308/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":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-23T01:11:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qy+HTIxGSBAo/a0hTwujRKr0xJaRUM+QZ/yTu5OJm2aR6DZG4x9ytq93JT69T3q4VpfUiYqps220C5VuDHzNAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T12:02:19.793155Z"},"content_sha256":"16311498f99b89abf3a92600562a16b85c82e03975a63fd5d26032e108dea028","schema_version":"1.0","event_id":"sha256:16311498f99b89abf3a92600562a16b85c82e03975a63fd5d26032e108dea028"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/bundle.json","state_url":"https://pith.science/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/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":"2026-07-04T12:02:19Z","links":{"resolver":"https://pith.science/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ","bundle":"https://pith.science/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/bundle.json","state":"https://pith.science/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PVM6SSWCTDHTHSXPQNDAVKNZHZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:PVM6SSWCTDHTHSXPQNDAVKNZHZ","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":"0a80df50beed5a04a4808b4a559602cdfabc9f82bcb3ba55daf542b8d62ceec6","cross_cats_sorted":["cond-mat.quant-gas","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-19T13:29:51Z","title_canon_sha256":"e91c09592e43214b5d3fe5124587625b3798b59b49362d20230554a4513aff36"},"schema_version":"1.0","source":{"id":"2506.16308","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.16308","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"arxiv_version","alias_value":"2506.16308v2","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.16308","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_12","alias_value":"PVM6SSWCTDHT","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_16","alias_value":"PVM6SSWCTDHTHSXP","created_at":"2026-06-23T01:11:55Z"},{"alias_kind":"pith_short_8","alias_value":"PVM6SSWC","created_at":"2026-06-23T01:11:55Z"}],"graph_snapshots":[{"event_id":"sha256:16311498f99b89abf3a92600562a16b85c82e03975a63fd5d26032e108dea028","target":"graph","created_at":"2026-06-23T01:11:55Z","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/2506.16308/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The non-Hermitian bulk-boundary correspondence features an interplay between the non-Hermitian skin effect and anomalous boundary-mode behavior. Whereas the skin effect is known to manifest itself in quantum dynamics in the form of chiral damping, it has remained less clear what impact the boundary modes may have. Here we derive experimentally accessible signatures of the boundary modes. We also establish clear criteria, based on the generalized Brillouin zone, that determine when bulk and boundary effects can be dynamically discerned using the Liouvillian separation gap. This leads to telltal","authors_text":"Emil J. Bergholtz, Fan Yang, Maria Zelenayova, Paolo Molignini","cross_cats":["cond-mat.quant-gas","physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-19T13:29:51Z","title":"Quantum dynamical signatures of non-Hermitian boundary modes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.16308","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:afd8cf4b25721bba2ee6c9299b6820b831f22564eda02bdf84217bec1fd60b67","target":"record","created_at":"2026-06-23T01:11:55Z","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":"0a80df50beed5a04a4808b4a559602cdfabc9f82bcb3ba55daf542b8d62ceec6","cross_cats_sorted":["cond-mat.quant-gas","physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-06-19T13:29:51Z","title_canon_sha256":"e91c09592e43214b5d3fe5124587625b3798b59b49362d20230554a4513aff36"},"schema_version":"1.0","source":{"id":"2506.16308","kind":"arxiv","version":2}},"canonical_sha256":"7d59e94ac298cf33caef83460aa9b93e59bc1836e81237cdb4f7dc4fb7500d9c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7d59e94ac298cf33caef83460aa9b93e59bc1836e81237cdb4f7dc4fb7500d9c","first_computed_at":"2026-06-23T01:11:55.888071Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-23T01:11:55.888071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5mqznSyjBCOd/koCh6cVBTcH5aeyGUOnb9pLbD8f8pLyz86RvlrU8BHTIQpPE69PbexLXNKGNVgVbnchmlFgBA==","signature_status":"signed_v1","signed_at":"2026-06-23T01:11:55.888574Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.16308","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:afd8cf4b25721bba2ee6c9299b6820b831f22564eda02bdf84217bec1fd60b67","sha256:16311498f99b89abf3a92600562a16b85c82e03975a63fd5d26032e108dea028"],"state_sha256":"f4da908dd801e4fff518f6dd8603c5e99b9547e87bfec1aad2e06d3ea8129c76"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qAFB0YOad3W4rcKRpSaRLQFtkSOhdE+c/LwGdzMXKjvCQN1PeZN0v+UyYNScLJjVh3K8Q0gPtaC+bkDuqok4Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-04T12:02:19.795082Z","bundle_sha256":"b127aee3fefd25b8d48f0392b7ebf9a441d0fae33f18de474059b31bbd1558c8"}}