{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:4HQPMPGFXQPU77K75LJUUGAQRG","short_pith_number":"pith:4HQPMPGF","canonical_record":{"source":{"id":"1801.04788","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-15T13:19:28Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"046ba1555e90778a01e7c574db8e037c108109504b72cb846b7f661db9bdaaff","abstract_canon_sha256":"54d8667d2bb002f57df207f3a8afbb8b50e274cad8f0730c1f204e09164d2e4c"},"schema_version":"1.0"},"canonical_sha256":"e1e0f63cc5bc1f4ffd5fead34a18108995c83d139eee39478f9088128c6e6991","source":{"kind":"arxiv","id":"1801.04788","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.04788","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"1801.04788v1","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.04788","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"4HQPMPGFXQPU","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"4HQPMPGFXQPU77K7","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"4HQPMPGF","created_at":"2026-05-18T12:32:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:4HQPMPGFXQPU77K75LJUUGAQRG","target":"record","payload":{"canonical_record":{"source":{"id":"1801.04788","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-15T13:19:28Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"046ba1555e90778a01e7c574db8e037c108109504b72cb846b7f661db9bdaaff","abstract_canon_sha256":"54d8667d2bb002f57df207f3a8afbb8b50e274cad8f0730c1f204e09164d2e4c"},"schema_version":"1.0"},"canonical_sha256":"e1e0f63cc5bc1f4ffd5fead34a18108995c83d139eee39478f9088128c6e6991","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:03.269038Z","signature_b64":"apRlZDBhdryhZvcOmb15EsXdy+xiyd6fpkFDmzPmULQtqOh3vlCri27llO65dfrmdSEG4UdGhjdIpverAmDjAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1e0f63cc5bc1f4ffd5fead34a18108995c83d139eee39478f9088128c6e6991","last_reissued_at":"2026-05-18T00:26:03.268349Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:03.268349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.04788","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":"2026-05-18T00:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LuLrcY3zovbYL1jeeCyDRNMc2tvIoBocMxJp8Ikb7IQmgz/CgkEkWNarwHt3uMxC4dFXx45yu9RhlMEAwaGKDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T07:58:07.383997Z"},"content_sha256":"38488b330d9164a4f4e1e799c7394a9b8905e2d2119999f1c545c63f047fb63a","schema_version":"1.0","event_id":"sha256:38488b330d9164a4f4e1e799c7394a9b8905e2d2119999f1c545c63f047fb63a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:4HQPMPGFXQPU77K75LJUUGAQRG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hybrid Interference Induced Flat Band Localization in Bipartite Optomechanical Lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Jin-Hua Gao, Liang-Liang Wan, Xin-You L\\\"u, Ying Wu","submitted_at":"2018-01-15T13:19:28Z","abstract_excerpt":"The flat band localization, as an important phenomenon in solid state physics, is fundamentally interesting in the exploration of exotic ground property of many-body system. Here we demonstrate the appearance of a flat band in a general bipartite optomechanical lattice, which could have one or two dimensional framework. Physically, it is induced by the hybrid interference between the photon and phonon modes in optomechanical lattice, which is quite different from the destructive interference resulted from the special geometry structure in the normal lattice (e.g., Lieb lattice). Moreover, this"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.04788","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":""},"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":"2026-05-18T00:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6h3z2qQu6l0VNx4mJhmQatZ7ZJBWstPLhK4tml95EOG+AixtvQ7bp13WK4cIXAYRdSnQI0CA2OOa5HHO6Pl/Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T07:58:07.384357Z"},"content_sha256":"1b3d79a5522e3907f0dff4b59aee7c173366155de3cc7d44c33cf3ea8f626de3","schema_version":"1.0","event_id":"sha256:1b3d79a5522e3907f0dff4b59aee7c173366155de3cc7d44c33cf3ea8f626de3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4HQPMPGFXQPU77K75LJUUGAQRG/bundle.json","state_url":"https://pith.science/pith/4HQPMPGFXQPU77K75LJUUGAQRG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4HQPMPGFXQPU77K75LJUUGAQRG/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":"2026-06-12T07:58:07Z","links":{"resolver":"https://pith.science/pith/4HQPMPGFXQPU77K75LJUUGAQRG","bundle":"https://pith.science/pith/4HQPMPGFXQPU77K75LJUUGAQRG/bundle.json","state":"https://pith.science/pith/4HQPMPGFXQPU77K75LJUUGAQRG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4HQPMPGFXQPU77K75LJUUGAQRG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:4HQPMPGFXQPU77K75LJUUGAQRG","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":"54d8667d2bb002f57df207f3a8afbb8b50e274cad8f0730c1f204e09164d2e4c","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-15T13:19:28Z","title_canon_sha256":"046ba1555e90778a01e7c574db8e037c108109504b72cb846b7f661db9bdaaff"},"schema_version":"1.0","source":{"id":"1801.04788","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.04788","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"1801.04788v1","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.04788","created_at":"2026-05-18T00:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"4HQPMPGFXQPU","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"4HQPMPGFXQPU77K7","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"4HQPMPGF","created_at":"2026-05-18T12:32:05Z"}],"graph_snapshots":[{"event_id":"sha256:1b3d79a5522e3907f0dff4b59aee7c173366155de3cc7d44c33cf3ea8f626de3","target":"graph","created_at":"2026-05-18T00:26:03Z","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"},"paper":{"abstract_excerpt":"The flat band localization, as an important phenomenon in solid state physics, is fundamentally interesting in the exploration of exotic ground property of many-body system. Here we demonstrate the appearance of a flat band in a general bipartite optomechanical lattice, which could have one or two dimensional framework. Physically, it is induced by the hybrid interference between the photon and phonon modes in optomechanical lattice, which is quite different from the destructive interference resulted from the special geometry structure in the normal lattice (e.g., Lieb lattice). Moreover, this","authors_text":"Jin-Hua Gao, Liang-Liang Wan, Xin-You L\\\"u, Ying Wu","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-15T13:19:28Z","title":"Hybrid Interference Induced Flat Band Localization in Bipartite Optomechanical Lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.04788","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":"sha256:38488b330d9164a4f4e1e799c7394a9b8905e2d2119999f1c545c63f047fb63a","target":"record","created_at":"2026-05-18T00:26:03Z","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":"54d8667d2bb002f57df207f3a8afbb8b50e274cad8f0730c1f204e09164d2e4c","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-01-15T13:19:28Z","title_canon_sha256":"046ba1555e90778a01e7c574db8e037c108109504b72cb846b7f661db9bdaaff"},"schema_version":"1.0","source":{"id":"1801.04788","kind":"arxiv","version":1}},"canonical_sha256":"e1e0f63cc5bc1f4ffd5fead34a18108995c83d139eee39478f9088128c6e6991","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e1e0f63cc5bc1f4ffd5fead34a18108995c83d139eee39478f9088128c6e6991","first_computed_at":"2026-05-18T00:26:03.268349Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:26:03.268349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"apRlZDBhdryhZvcOmb15EsXdy+xiyd6fpkFDmzPmULQtqOh3vlCri27llO65dfrmdSEG4UdGhjdIpverAmDjAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:26:03.269038Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.04788","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:38488b330d9164a4f4e1e799c7394a9b8905e2d2119999f1c545c63f047fb63a","sha256:1b3d79a5522e3907f0dff4b59aee7c173366155de3cc7d44c33cf3ea8f626de3"],"state_sha256":"d6dfee1218f48c771c2fc0216ab0566ed9567e2ffbf51eb8be6f35992aa05de8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UjsHaV6SteLBc6+J8DZroVgbfu4q5rel23tdhtNDWZeNWUaPLqkYy6MWFznQG+kJOI0jj6m7k1Scjpz5MIGSAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T07:58:07.386371Z","bundle_sha256":"83b66d43c44a6cfe9b3d2b82c3c51a4ceb66760be5c936bec23886b1ae3e051b"}}