{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:Q4VUL23AVYB3GYRXTD3P56CXOC","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":"3c7e49226c05dd1579ea204af96035f4d447757161f85e693d6fd087bbd81ff1","cross_cats_sorted":["cond-mat.other"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-03-14T21:22:05Z","title_canon_sha256":"e2b3b1749d8be84e71b493900850bfd67c1e6365b0eba70982fd0f951f57cd2a"},"schema_version":"1.0","source":{"id":"2503.11885","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2503.11885","created_at":"2026-07-05T11:31:44Z"},{"alias_kind":"arxiv_version","alias_value":"2503.11885v1","created_at":"2026-07-05T11:31:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.11885","created_at":"2026-07-05T11:31:44Z"},{"alias_kind":"pith_short_12","alias_value":"Q4VUL23AVYB3","created_at":"2026-07-05T11:31:44Z"},{"alias_kind":"pith_short_16","alias_value":"Q4VUL23AVYB3GYRX","created_at":"2026-07-05T11:31:44Z"},{"alias_kind":"pith_short_8","alias_value":"Q4VUL23A","created_at":"2026-07-05T11:31:44Z"}],"graph_snapshots":[{"event_id":"sha256:4d572afddc41bb87d7fb925b7495d6dac59e29703d4b85ac352252ada741e34a","target":"graph","created_at":"2026-07-05T11:31:44Z","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/2503.11885/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In spaces of three or more dimensions, there exists topological physics of significant richness that has no lower-dimensional counterparts. To experimentally explore high-dimensional physics, it is advantageous to augment the physical space with synthetic dimensions. An emerging approach is to use a single modulated photonic ring resonator to form multiple synthetic frequency dimensions. However, all the high-dimensional Hamiltonians experimentally demonstrated in this approach are topologically trivial. Here we propose a general scheme to create high-dimensional topological physics using mult","authors_text":"Charles Roques-Carmes, Dali Cheng, Heming Wang, Janet Zhong, Shanhui Fan","cross_cats":["cond-mat.other"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-03-14T21:22:05Z","title":"Creating high-dimensional topological physics using a single ring resonator"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.11885","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:fbe80ac2daba109db11118c1b3322a1a5079d2bf7a14f38448e30c59cb8a84b6","target":"record","created_at":"2026-07-05T11:31:44Z","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":"3c7e49226c05dd1579ea204af96035f4d447757161f85e693d6fd087bbd81ff1","cross_cats_sorted":["cond-mat.other"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-03-14T21:22:05Z","title_canon_sha256":"e2b3b1749d8be84e71b493900850bfd67c1e6365b0eba70982fd0f951f57cd2a"},"schema_version":"1.0","source":{"id":"2503.11885","kind":"arxiv","version":1}},"canonical_sha256":"872b45eb60ae03b3623798f6fef85770a9ed90d144bcb079b5b2555951af240e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"872b45eb60ae03b3623798f6fef85770a9ed90d144bcb079b5b2555951af240e","first_computed_at":"2026-07-05T11:31:44.256011Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:31:44.256011Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"o5JUmT96in3iDzxyBw6pjXyEd+S3cRbQmRX2vAqqJOHle0boUH0zvZ0gllxR33Hnk0L2qCxIW411AeVww/rcBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:31:44.256522Z","signed_message":"canonical_sha256_bytes"},"source_id":"2503.11885","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fbe80ac2daba109db11118c1b3322a1a5079d2bf7a14f38448e30c59cb8a84b6","sha256:4d572afddc41bb87d7fb925b7495d6dac59e29703d4b85ac352252ada741e34a"],"state_sha256":"b46725f6e7ceba2338d3a0290dd56a9ce44a0b614e3ea22cb70a2cd63a7f878d"}