{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:F3K2IQ34C3XZCR76A234TOCZM4","short_pith_number":"pith:F3K2IQ34","canonical_record":{"source":{"id":"1504.04014","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-15T20:00:35Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"bd9d0b9361daf3f2bddab3743296357de96ed406c8715fecc7f2912a35cbe615","abstract_canon_sha256":"d10131d2f5fd423e1426a1420fdf2ed59a17d63dd15688d39745c5f248017301"},"schema_version":"1.0"},"canonical_sha256":"2ed5a4437c16ef9147fe06b7c9b859670c524896b6da6dfac712df29d307f728","source":{"kind":"arxiv","id":"1504.04014","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.04014","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"arxiv_version","alias_value":"1504.04014v2","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.04014","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"pith_short_12","alias_value":"F3K2IQ34C3XZ","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_16","alias_value":"F3K2IQ34C3XZCR76","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_8","alias_value":"F3K2IQ34","created_at":"2026-05-18T12:29:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:F3K2IQ34C3XZCR76A234TOCZM4","target":"record","payload":{"canonical_record":{"source":{"id":"1504.04014","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-15T20:00:35Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"bd9d0b9361daf3f2bddab3743296357de96ed406c8715fecc7f2912a35cbe615","abstract_canon_sha256":"d10131d2f5fd423e1426a1420fdf2ed59a17d63dd15688d39745c5f248017301"},"schema_version":"1.0"},"canonical_sha256":"2ed5a4437c16ef9147fe06b7c9b859670c524896b6da6dfac712df29d307f728","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:32:10.406974Z","signature_b64":"GvG+xsrjrbKCwBL0tNNfzRB54yoeCJc3mlkyFJVXZ03uSGBb6yKeY74/tI6uJe33IrRxhan7iJCiBMSenBFJDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ed5a4437c16ef9147fe06b7c9b859670c524896b6da6dfac712df29d307f728","last_reissued_at":"2026-05-18T01:32:10.406285Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:32:10.406285Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1504.04014","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":"2026-05-18T01:32:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jTTHwaupmh5/E9p/2lGCxD4gg/e0wnnTzu8myBqY43KUsJog2tKjBq2STPeUZk4iETFgUMn0AIRv5iS+l5jbCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T09:35:15.935498Z"},"content_sha256":"532ce3849332aa2c087e07e1f7779c84835160b9676bf650976469054ee4fd25","schema_version":"1.0","event_id":"sha256:532ce3849332aa2c087e07e1f7779c84835160b9676bf650976469054ee4fd25"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:F3K2IQ34C3XZCR76A234TOCZM4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"How to directly observe Landau levels in driven-dissipative strained honeycomb lattices","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"cond-mat.quant-gas","authors_text":"Grazia Salerno, Hannah M. Price, Iacopo Carusotto, Tomoki Ozawa","submitted_at":"2015-04-15T20:00:35Z","abstract_excerpt":"We study the driven-dissipative steady-state of a coherently-driven Bose field in a honeycomb lattice geometry. In the presence of a suitable spatial modulation of the hopping amplitudes, a valley-dependent artificial magnetic field appears and the low-energy eigenmodes have the form of relativistic Landau levels. We show how the main properties of the Landau levels can be extracted by observing the peaks in the absorption spectrum of the system and the corresponding spatial intensity distribution. Finally, quantitative predictions for realistic lattices based on photonic or microwave technolo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.04014","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":""},"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":"2026-05-18T01:32:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w/P/T5x1EhUnPxTnfXomPhqqXo4FGzBm7GpsHnZhpu6jGcSl9uCgpNh0itXqFW3v2m/Jc1nuiTI8G9yUvYNVAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T09:35:15.935842Z"},"content_sha256":"1e518e0978a82c1bad976a52d2dc9107aea6fc991944c082306bb62efafdb697","schema_version":"1.0","event_id":"sha256:1e518e0978a82c1bad976a52d2dc9107aea6fc991944c082306bb62efafdb697"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/F3K2IQ34C3XZCR76A234TOCZM4/bundle.json","state_url":"https://pith.science/pith/F3K2IQ34C3XZCR76A234TOCZM4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/F3K2IQ34C3XZCR76A234TOCZM4/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":"2026-06-01T09:35:15Z","links":{"resolver":"https://pith.science/pith/F3K2IQ34C3XZCR76A234TOCZM4","bundle":"https://pith.science/pith/F3K2IQ34C3XZCR76A234TOCZM4/bundle.json","state":"https://pith.science/pith/F3K2IQ34C3XZCR76A234TOCZM4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/F3K2IQ34C3XZCR76A234TOCZM4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:F3K2IQ34C3XZCR76A234TOCZM4","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":"d10131d2f5fd423e1426a1420fdf2ed59a17d63dd15688d39745c5f248017301","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-15T20:00:35Z","title_canon_sha256":"bd9d0b9361daf3f2bddab3743296357de96ed406c8715fecc7f2912a35cbe615"},"schema_version":"1.0","source":{"id":"1504.04014","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.04014","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"arxiv_version","alias_value":"1504.04014v2","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.04014","created_at":"2026-05-18T01:32:10Z"},{"alias_kind":"pith_short_12","alias_value":"F3K2IQ34C3XZ","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_16","alias_value":"F3K2IQ34C3XZCR76","created_at":"2026-05-18T12:29:19Z"},{"alias_kind":"pith_short_8","alias_value":"F3K2IQ34","created_at":"2026-05-18T12:29:19Z"}],"graph_snapshots":[{"event_id":"sha256:1e518e0978a82c1bad976a52d2dc9107aea6fc991944c082306bb62efafdb697","target":"graph","created_at":"2026-05-18T01:32:10Z","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":"We study the driven-dissipative steady-state of a coherently-driven Bose field in a honeycomb lattice geometry. In the presence of a suitable spatial modulation of the hopping amplitudes, a valley-dependent artificial magnetic field appears and the low-energy eigenmodes have the form of relativistic Landau levels. We show how the main properties of the Landau levels can be extracted by observing the peaks in the absorption spectrum of the system and the corresponding spatial intensity distribution. Finally, quantitative predictions for realistic lattices based on photonic or microwave technolo","authors_text":"Grazia Salerno, Hannah M. Price, Iacopo Carusotto, Tomoki Ozawa","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-15T20:00:35Z","title":"How to directly observe Landau levels in driven-dissipative strained honeycomb lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.04014","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":"sha256:532ce3849332aa2c087e07e1f7779c84835160b9676bf650976469054ee4fd25","target":"record","created_at":"2026-05-18T01:32:10Z","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":"d10131d2f5fd423e1426a1420fdf2ed59a17d63dd15688d39745c5f248017301","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-04-15T20:00:35Z","title_canon_sha256":"bd9d0b9361daf3f2bddab3743296357de96ed406c8715fecc7f2912a35cbe615"},"schema_version":"1.0","source":{"id":"1504.04014","kind":"arxiv","version":2}},"canonical_sha256":"2ed5a4437c16ef9147fe06b7c9b859670c524896b6da6dfac712df29d307f728","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2ed5a4437c16ef9147fe06b7c9b859670c524896b6da6dfac712df29d307f728","first_computed_at":"2026-05-18T01:32:10.406285Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:32:10.406285Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GvG+xsrjrbKCwBL0tNNfzRB54yoeCJc3mlkyFJVXZ03uSGBb6yKeY74/tI6uJe33IrRxhan7iJCiBMSenBFJDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:32:10.406974Z","signed_message":"canonical_sha256_bytes"},"source_id":"1504.04014","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:532ce3849332aa2c087e07e1f7779c84835160b9676bf650976469054ee4fd25","sha256:1e518e0978a82c1bad976a52d2dc9107aea6fc991944c082306bb62efafdb697"],"state_sha256":"7121dce2b096ec5504104c66d14d174c74635be65fb20b1188d158f1f4dc0a9b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"etjE5tqoJSQaeMeVfK40rbVTt71urjBnzHTrDXACVjKP3MRWeN2/wjnBQJ+lPCKo/5QNP2e+byzIpkH8Q3KhCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T09:35:15.937826Z","bundle_sha256":"2bd1175f0d24f5c8f2d519d7787578395a78638bf11f6d7963cb7e4187678075"}}