{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6EN5OZV3DXN2LBFHBL3YTXPPSS","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":"3b44633e4e31a61cc07463b25bcc124a621c08b8b988892df4740b545ee72353","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-24T08:45:11Z","title_canon_sha256":"de6c8fdb23b52238bbebd8b8c80c8389b3eb800d71d1bce28097a0abacf8b32c"},"schema_version":"1.0","source":{"id":"1411.6380","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.6380","created_at":"2026-05-18T02:04:08Z"},{"alias_kind":"arxiv_version","alias_value":"1411.6380v1","created_at":"2026-05-18T02:04:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.6380","created_at":"2026-05-18T02:04:08Z"},{"alias_kind":"pith_short_12","alias_value":"6EN5OZV3DXN2","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6EN5OZV3DXN2LBFH","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6EN5OZV3","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:33593a2262e3174e5770f3bd202a37ddb645be177c404fefcdc5e9348c1bca24","target":"graph","created_at":"2026-05-18T02:04:08Z","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":"Multi-cavity photonic systems, known as photonic molecules (PMs), are ideal multi-well potential building blocks for advanced quantum and nonlinear optics. A key phenomenon arising in double well potentials is the spontaneous breaking of the inversion symmetry, i.e. a transition from a delocalized to two localized states in the wells, which are mirror images of each other. Although few theoretical studies have addressed mirror-symmetry breaking in micro and nanophotonic systems, no experimental evidence has been reported to date. Thanks to the potential barrier engineering implemented here, we","authors_text":"Alejandro M. Yacomotti, Ariel Levenson, Fabrice Raineri, Gregoire Beaudoin, Isabelle Sagnes, Paul Monnier, Philippe Hamel, Samir Haddadi","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-24T08:45:11Z","title":"Spontaneous mirror-symmetry breaking in a photonic molecule"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.6380","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":"sha256:411e4dbd1507b9bfdb83aae35113a575e7a33c4e8c7817845371dadb054be716","target":"record","created_at":"2026-05-18T02:04:08Z","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":"3b44633e4e31a61cc07463b25bcc124a621c08b8b988892df4740b545ee72353","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-24T08:45:11Z","title_canon_sha256":"de6c8fdb23b52238bbebd8b8c80c8389b3eb800d71d1bce28097a0abacf8b32c"},"schema_version":"1.0","source":{"id":"1411.6380","kind":"arxiv","version":1}},"canonical_sha256":"f11bd766bb1ddba584a70af789ddef94a915011f0f0cc045b6f5f0f9dc138d12","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f11bd766bb1ddba584a70af789ddef94a915011f0f0cc045b6f5f0f9dc138d12","first_computed_at":"2026-05-18T02:04:08.196406Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:08.196406Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Lr0sHsDwI1nBEimdlQjhGwE1WoyI3aTn0VKtoSTgYfEuW7pQ8vDF4wlOrj/SWmd/WDddf5aVzgWyYJ1b0bcADw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:08.197216Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.6380","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:411e4dbd1507b9bfdb83aae35113a575e7a33c4e8c7817845371dadb054be716","sha256:33593a2262e3174e5770f3bd202a37ddb645be177c404fefcdc5e9348c1bca24"],"state_sha256":"4acfd236766d015f59a8b1e043a711a7bfa57d3f2f8866232a73c3599bc2d746"}