{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:QPVZKAN37KCNMWKPGDU75TS4VJ","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":"341b93bfa1076dd49756d0da700545b25351c0d1a7f613d1656a913e9c94865d","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-03-10T11:09:31Z","title_canon_sha256":"e994de18fa569efab5119bcfd08b490ba2bbba8f1b6da11bc7678755079a7ba2"},"schema_version":"1.0","source":{"id":"2203.05289","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2203.05289","created_at":"2026-07-05T05:18:02Z"},{"alias_kind":"arxiv_version","alias_value":"2203.05289v1","created_at":"2026-07-05T05:18:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.05289","created_at":"2026-07-05T05:18:02Z"},{"alias_kind":"pith_short_12","alias_value":"QPVZKAN37KCN","created_at":"2026-07-05T05:18:02Z"},{"alias_kind":"pith_short_16","alias_value":"QPVZKAN37KCNMWKP","created_at":"2026-07-05T05:18:02Z"},{"alias_kind":"pith_short_8","alias_value":"QPVZKAN3","created_at":"2026-07-05T05:18:02Z"}],"graph_snapshots":[{"event_id":"sha256:31aeaee686ce9866f9a0a26d163390219cd5aaa9322eb8eec7f611b769530589","target":"graph","created_at":"2026-07-05T05:18:02Z","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/2203.05289/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The field of spinoptronics is underpinned by good control over photonic spin-orbit coupling in devices that possess strong optical nonlinearities. Such devices might hold the key to a new era of optoelectronics where momentum and polarization degrees-of-freedom of light are interwoven and interfaced with electronics. However, manipulating photons through electrical means is a daunting task given their charge neutrality and requires complex electro-optic modulation of their medium. In this work, we present electrically tunable microcavity exciton-polariton resonances in a Rashba-Dresselhaus spi","authors_text":"A. Wincukiewicz, B. Pi\\k{e}tka, D. Ballarini, D. Sanvitto, H. Sigurdsson, J. Szczytko, K. {\\L}empicka-Mirek, L. De Marco, M. Kami\\'nska, M. Kr\\'ol, M. Muszy\\'nski, P.G. Lagoudakis, P. Kula, P. Morawiak, R. Mazur, T. Stefaniuk, W. Piecek","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-03-10T11:09:31Z","title":"Electrically tunable Berry curvature and strong light-matter coupling in birefringent perovskite microcavities at room temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.05289","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:d60285b71d67dc8dd948cba5fe38a28f3697ad53c6c889684c1a05881806fdf1","target":"record","created_at":"2026-07-05T05:18:02Z","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":"341b93bfa1076dd49756d0da700545b25351c0d1a7f613d1656a913e9c94865d","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2022-03-10T11:09:31Z","title_canon_sha256":"e994de18fa569efab5119bcfd08b490ba2bbba8f1b6da11bc7678755079a7ba2"},"schema_version":"1.0","source":{"id":"2203.05289","kind":"arxiv","version":1}},"canonical_sha256":"83eb9501bbfa84d6594f30e9fece5caa71b37f66f0d7a0dc0018b424fb6c0924","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"83eb9501bbfa84d6594f30e9fece5caa71b37f66f0d7a0dc0018b424fb6c0924","first_computed_at":"2026-07-05T05:18:02.191932Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:18:02.191932Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MeybMRnRcRBs9uiwp6ISqzG7zb8es0S5Xl3/Hb9/O8vEmd/TWU4FDEZ5Qm6uImzUUUzJ8W6ewZnW0K+yxYE2AQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:18:02.192501Z","signed_message":"canonical_sha256_bytes"},"source_id":"2203.05289","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d60285b71d67dc8dd948cba5fe38a28f3697ad53c6c889684c1a05881806fdf1","sha256:31aeaee686ce9866f9a0a26d163390219cd5aaa9322eb8eec7f611b769530589"],"state_sha256":"f95cafd68f582600152dd7eb47545f86faa1d9865c1bdd76594f0840357ba333"}