{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:3A34U3SVBKWQZ6DZ25WJVCD765","short_pith_number":"pith:3A34U3SV","canonical_record":{"source":{"id":"2607.06267","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-07T13:32:46Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"title_canon_sha256":"17c32e0b373e67e399c7c0352bed2996cb20ce90f460dc1a5d30df77051dbd22","abstract_canon_sha256":"57fe47d6e6e7ae482cfc1041cd16fda45e32edeb3971a6f93c081d629381cfe9"},"schema_version":"1.0"},"canonical_sha256":"d837ca6e550aad0cf879d76c9a887ff75b8ce0a9873e670a0fc3084054ba796a","source":{"kind":"arxiv","id":"2607.06267","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.06267","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"arxiv_version","alias_value":"2607.06267v1","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.06267","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_12","alias_value":"3A34U3SVBKWQ","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_16","alias_value":"3A34U3SVBKWQZ6DZ","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_8","alias_value":"3A34U3SV","created_at":"2026-07-08T01:19:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:3A34U3SVBKWQZ6DZ25WJVCD765","target":"record","payload":{"canonical_record":{"source":{"id":"2607.06267","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-07T13:32:46Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"title_canon_sha256":"17c32e0b373e67e399c7c0352bed2996cb20ce90f460dc1a5d30df77051dbd22","abstract_canon_sha256":"57fe47d6e6e7ae482cfc1041cd16fda45e32edeb3971a6f93c081d629381cfe9"},"schema_version":"1.0"},"canonical_sha256":"d837ca6e550aad0cf879d76c9a887ff75b8ce0a9873e670a0fc3084054ba796a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-08T01:19:19.468236Z","signature_b64":"K9vGtJm3sRdSKteA/alXzkU8xJAPTS6mvUIxTP0QG0Ob43YurECoSV652oPvICiy2zTCg4snYFTUVfeneScvBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d837ca6e550aad0cf879d76c9a887ff75b8ce0a9873e670a0fc3084054ba796a","last_reissued_at":"2026-07-08T01:19:19.467746Z","signature_status":"signed_v1","first_computed_at":"2026-07-08T01:19:19.467746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2607.06267","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":"2026-07-08T01:19:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xSB+dLNeHTlBIJ09b0Us1hv3mq8Yxt1o6HMvNsRr/AIsX3yOiG22GDGatpAFwo1nJ6O6AJPR1pbQNjKl46zRDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T18:08:59.128014Z"},"content_sha256":"1bbfb641f7bbfdffafde44e263baa49d259c8b20ed8d25ee15540358687bc8bf","schema_version":"1.0","event_id":"sha256:1bbfb641f7bbfdffafde44e263baa49d259c8b20ed8d25ee15540358687bc8bf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:3A34U3SVBKWQZ6DZ25WJVCD765","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral Graviton Modes in Non-Abelian lattice Fractional Quantum Hall states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Hernan Xavier, Hongyu Lu, Marcello Dalmonte, Min Long, Zeno Bacciconi, Zi Yang Meng","submitted_at":"2026-07-07T13:32:46Z","abstract_excerpt":"Synthetic quantum matter provides a highly tunable route to fractional quantum Hall physics beyond the constraints of conventional electronic materials. However, previous theoretical studies have mostly focused on their ground state properties. It remains unclear to what extent such platforms could reveal key excitation properties of fractional quantum Hall states. Here, we study charge-neutral collective excitations in a non-abelian lattice fractional quantum Hall state realized in the bosonic Harper-Hofstadter model at unity filling factior, realizing a Moore-Read ground state. Combining ful"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.06267","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.06267/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":"2026-07-08T01:19:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nGetzJO8aB3ZTShRQ5HlX6FvoSsNfTz9dVRskX588+r/jb1YasNmFz3UUtVE9cDMonOobchzaU8nbHzxHWCxCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T18:08:59.128522Z"},"content_sha256":"93c9ed04301f5d1c741d12ea827ccab2c4e424b9aa5a3b0860e57ff2210d0434","schema_version":"1.0","event_id":"sha256:93c9ed04301f5d1c741d12ea827ccab2c4e424b9aa5a3b0860e57ff2210d0434"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:3A34U3SVBKWQZ6DZ25WJVCD765","target":"integrity","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1103/phys-revb.86.245107) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"H. N. Phien, G. Vidal, and I. P. McCulloch, In- finite boundary conditions for matrix product state calculations, Physical Review B86, 10.1103/phys- revb.86.245107 (2012)","arxiv_id":"2607.06267","detector":"doi_compliance","evidence":{"ref_index":60,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"H. N. Phien, G. Vidal, and I. P. McCulloch, In- finite boundary conditions for matrix product state calculations, Physical Review B86, 10.1103/phys- revb.86.245107 (2012)","reconstructed_doi":"10.1103/phys-revb.86.245107"},"severity":"advisory","ref_index":60,"audited_at":"2026-07-09T07:35:14.570982Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/phys-revb.86.245107","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"77231d6f527cb9370468419b7c0baff08ef8a1442d9a26afd4172d2ab62a3b34","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.0.0","detected_arxiv_id":null,"integrity_event_id":7803,"payload_sha256":"ec462e80d0cfd7007ee320ba94726f41d355d5435ed48dbfb53502bdc8987f87","signature_b64":"Eq7oXygih2YbG16+9ONFJANK8cHbRkXJQvfAjiXYtRMy2LFED5qGjybsAUucqP+qSWJ7/SNFmTPh6cgdsXg4Dw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-09T07:37:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nRG6ErFzdHo1+vvbwlYFkg3wrDsihgEkEi2tMCK5X866UVgnkDRYIAhaVGyvHRYZUG2XfvulfTE5Q1g8wC53DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T18:08:59.131383Z"},"content_sha256":"dadb7aa0f47a7929d3a5687945f0ed4119bb251eddf7756de3e91524caa9fd61","schema_version":"1.0","event_id":"sha256:dadb7aa0f47a7929d3a5687945f0ed4119bb251eddf7756de3e91524caa9fd61"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3A34U3SVBKWQZ6DZ25WJVCD765/bundle.json","state_url":"https://pith.science/pith/3A34U3SVBKWQZ6DZ25WJVCD765/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3A34U3SVBKWQZ6DZ25WJVCD765/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":"2026-08-07T18:08:59Z","links":{"resolver":"https://pith.science/pith/3A34U3SVBKWQZ6DZ25WJVCD765","bundle":"https://pith.science/pith/3A34U3SVBKWQZ6DZ25WJVCD765/bundle.json","state":"https://pith.science/pith/3A34U3SVBKWQZ6DZ25WJVCD765/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3A34U3SVBKWQZ6DZ25WJVCD765/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:3A34U3SVBKWQZ6DZ25WJVCD765","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"57fe47d6e6e7ae482cfc1041cd16fda45e32edeb3971a6f93c081d629381cfe9","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-07T13:32:46Z","title_canon_sha256":"17c32e0b373e67e399c7c0352bed2996cb20ce90f460dc1a5d30df77051dbd22"},"schema_version":"1.0","source":{"id":"2607.06267","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.06267","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"arxiv_version","alias_value":"2607.06267v1","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.06267","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_12","alias_value":"3A34U3SVBKWQ","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_16","alias_value":"3A34U3SVBKWQZ6DZ","created_at":"2026-07-08T01:19:19Z"},{"alias_kind":"pith_short_8","alias_value":"3A34U3SV","created_at":"2026-07-08T01:19:19Z"}],"graph_snapshots":[{"event_id":"sha256:93c9ed04301f5d1c741d12ea827ccab2c4e424b9aa5a3b0860e57ff2210d0434","target":"graph","created_at":"2026-07-08T01:19:19Z","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/2607.06267/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Synthetic quantum matter provides a highly tunable route to fractional quantum Hall physics beyond the constraints of conventional electronic materials. However, previous theoretical studies have mostly focused on their ground state properties. It remains unclear to what extent such platforms could reveal key excitation properties of fractional quantum Hall states. Here, we study charge-neutral collective excitations in a non-abelian lattice fractional quantum Hall state realized in the bosonic Harper-Hofstadter model at unity filling factior, realizing a Moore-Read ground state. Combining ful","authors_text":"Hernan Xavier, Hongyu Lu, Marcello Dalmonte, Min Long, Zeno Bacciconi, Zi Yang Meng","cross_cats":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-07T13:32:46Z","title":"Chiral Graviton Modes in Non-Abelian lattice Fractional Quantum Hall states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.06267","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":"sha256:1bbfb641f7bbfdffafde44e263baa49d259c8b20ed8d25ee15540358687bc8bf","target":"record","created_at":"2026-07-08T01:19:19Z","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":"57fe47d6e6e7ae482cfc1041cd16fda45e32edeb3971a6f93c081d629381cfe9","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-07T13:32:46Z","title_canon_sha256":"17c32e0b373e67e399c7c0352bed2996cb20ce90f460dc1a5d30df77051dbd22"},"schema_version":"1.0","source":{"id":"2607.06267","kind":"arxiv","version":1}},"canonical_sha256":"d837ca6e550aad0cf879d76c9a887ff75b8ce0a9873e670a0fc3084054ba796a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d837ca6e550aad0cf879d76c9a887ff75b8ce0a9873e670a0fc3084054ba796a","first_computed_at":"2026-07-08T01:19:19.467746Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-08T01:19:19.467746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"K9vGtJm3sRdSKteA/alXzkU8xJAPTS6mvUIxTP0QG0Ob43YurECoSV652oPvICiy2zTCg4snYFTUVfeneScvBg==","signature_status":"signed_v1","signed_at":"2026-07-08T01:19:19.468236Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.06267","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1bbfb641f7bbfdffafde44e263baa49d259c8b20ed8d25ee15540358687bc8bf","sha256:93c9ed04301f5d1c741d12ea827ccab2c4e424b9aa5a3b0860e57ff2210d0434","sha256:dadb7aa0f47a7929d3a5687945f0ed4119bb251eddf7756de3e91524caa9fd61"],"state_sha256":"3b31ce158972081c1f454a4e1d00c453e86ddf78268588fda52cdad60df2ffd7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+ZnT4YU+nagQQ48GFQ4KioIDPSsqsMsFrJPbPTrxuNwNttY9BOVB4ZSQigRbn9/chBH8CrrZ0SdYoIcB9kmFAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T18:08:59.133553Z","bundle_sha256":"8912a3b70445caffdbfaeda1a5746df90c43849ae7d62fb4d166398ef9697142"}}