{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:U2RGJOHEHCQSHDHCCVW6TQSEFD","short_pith_number":"pith:U2RGJOHE","canonical_record":{"source":{"id":"2505.24800","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-30T17:03:07Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"fa1f10e09d431821c621b74bd8642d4275819db6ecd2c806de8cb360815dfb5c","abstract_canon_sha256":"4d9c0098f63d5cc84f1b59b25c3891057b931e1d8296476571a8b4e7b3dbfa3e"},"schema_version":"1.0"},"canonical_sha256":"a6a264b8e438a1238ce2156de9c24428e78c49e84893fcdf38202c37b6c26692","source":{"kind":"arxiv","id":"2505.24800","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.24800","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"arxiv_version","alias_value":"2505.24800v1","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24800","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_12","alias_value":"U2RGJOHEHCQS","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_16","alias_value":"U2RGJOHEHCQSHDHC","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_8","alias_value":"U2RGJOHE","created_at":"2026-07-05T11:12:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:U2RGJOHEHCQSHDHCCVW6TQSEFD","target":"record","payload":{"canonical_record":{"source":{"id":"2505.24800","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-30T17:03:07Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"fa1f10e09d431821c621b74bd8642d4275819db6ecd2c806de8cb360815dfb5c","abstract_canon_sha256":"4d9c0098f63d5cc84f1b59b25c3891057b931e1d8296476571a8b4e7b3dbfa3e"},"schema_version":"1.0"},"canonical_sha256":"a6a264b8e438a1238ce2156de9c24428e78c49e84893fcdf38202c37b6c26692","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:12:56.869976Z","signature_b64":"kS8nd09DmmPt+wcgJBqrL6MgTb6cfAjep/NdaGfHnwGUDWrc0Ol2beIu5Ikz0SzcAW46F2HY7/GglRUtBXUCCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a6a264b8e438a1238ce2156de9c24428e78c49e84893fcdf38202c37b6c26692","last_reissued_at":"2026-07-05T11:12:56.869471Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:12:56.869471Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2505.24800","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":"2026-07-05T11:12:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u8X1cEyCJUJ7qxmuHY+vfASUA9owd4/wXpbxRrWWJz+0lw/GEcs75ltvgMOxrJTHT5lqp0BFFvkd2k9ePVDHCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T01:15:26.743104Z"},"content_sha256":"62aa08da20369c047b311f6060e50ba84b333c3080b6f9dd14fd9d35a2069705","schema_version":"1.0","event_id":"sha256:62aa08da20369c047b311f6060e50ba84b333c3080b6f9dd14fd9d35a2069705"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:U2RGJOHEHCQSHDHCCVW6TQSEFD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strong coupling of chiral light with chiral matter: a macroscopic study","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"physics.optics","authors_text":"Denis G. Baranov, Ilia A. Smagin, Ilia M. Fradkin, Natalia S. Salakhova, Nikolay A. Gippius, Oleg Blokhin, Sergey A. Dyakov","submitted_at":"2025-05-30T17:03:07Z","abstract_excerpt":"Maximizing the interaction between chiral light and chiral matter is pivotal for the advancement of technologies enabling optical detection that distinguishes between different handedness in chiral organic molecules. One strategy involves developing a resonator that sustains photonic modes with non-zero electromagnetic handedness, which interact differently with chiral molecules of opposite enantiomers. When chiral molecules are positioned in resonator hotspots, they can alter the system's characteristics due to their inherent electric and magnetic transition dipole moments. In this study, we "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24800","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.24800/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T11:12:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"InklHb0yCFhK7dLrUVaJtob1X/LwOJSSi42X1dCBJ1f/Vv7Lt1ADkCRxgUWAp7B8X1rL/JnoNhDy0yAjMDc8DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T01:15:26.743571Z"},"content_sha256":"260ffb6b2059e21a1999f0b2cbc320d508b055cecd4641a3e3154e75fcbaebdd","schema_version":"1.0","event_id":"sha256:260ffb6b2059e21a1999f0b2cbc320d508b055cecd4641a3e3154e75fcbaebdd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/bundle.json","state_url":"https://pith.science/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/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":"2026-08-08T01:15:26Z","links":{"resolver":"https://pith.science/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD","bundle":"https://pith.science/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/bundle.json","state":"https://pith.science/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/U2RGJOHEHCQSHDHCCVW6TQSEFD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:U2RGJOHEHCQSHDHCCVW6TQSEFD","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":"4d9c0098f63d5cc84f1b59b25c3891057b931e1d8296476571a8b4e7b3dbfa3e","cross_cats_sorted":["cond-mat.other"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-30T17:03:07Z","title_canon_sha256":"fa1f10e09d431821c621b74bd8642d4275819db6ecd2c806de8cb360815dfb5c"},"schema_version":"1.0","source":{"id":"2505.24800","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.24800","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"arxiv_version","alias_value":"2505.24800v1","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24800","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_12","alias_value":"U2RGJOHEHCQS","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_16","alias_value":"U2RGJOHEHCQSHDHC","created_at":"2026-07-05T11:12:56Z"},{"alias_kind":"pith_short_8","alias_value":"U2RGJOHE","created_at":"2026-07-05T11:12:56Z"}],"graph_snapshots":[{"event_id":"sha256:260ffb6b2059e21a1999f0b2cbc320d508b055cecd4641a3e3154e75fcbaebdd","target":"graph","created_at":"2026-07-05T11:12:56Z","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/2505.24800/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Maximizing the interaction between chiral light and chiral matter is pivotal for the advancement of technologies enabling optical detection that distinguishes between different handedness in chiral organic molecules. One strategy involves developing a resonator that sustains photonic modes with non-zero electromagnetic handedness, which interact differently with chiral molecules of opposite enantiomers. When chiral molecules are positioned in resonator hotspots, they can alter the system's characteristics due to their inherent electric and magnetic transition dipole moments. In this study, we ","authors_text":"Denis G. Baranov, Ilia A. Smagin, Ilia M. Fradkin, Natalia S. Salakhova, Nikolay A. Gippius, Oleg Blokhin, Sergey A. Dyakov","cross_cats":["cond-mat.other"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-30T17:03:07Z","title":"Strong coupling of chiral light with chiral matter: a macroscopic study"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24800","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":"sha256:62aa08da20369c047b311f6060e50ba84b333c3080b6f9dd14fd9d35a2069705","target":"record","created_at":"2026-07-05T11:12:56Z","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":"4d9c0098f63d5cc84f1b59b25c3891057b931e1d8296476571a8b4e7b3dbfa3e","cross_cats_sorted":["cond-mat.other"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.optics","submitted_at":"2025-05-30T17:03:07Z","title_canon_sha256":"fa1f10e09d431821c621b74bd8642d4275819db6ecd2c806de8cb360815dfb5c"},"schema_version":"1.0","source":{"id":"2505.24800","kind":"arxiv","version":1}},"canonical_sha256":"a6a264b8e438a1238ce2156de9c24428e78c49e84893fcdf38202c37b6c26692","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a6a264b8e438a1238ce2156de9c24428e78c49e84893fcdf38202c37b6c26692","first_computed_at":"2026-07-05T11:12:56.869471Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:12:56.869471Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kS8nd09DmmPt+wcgJBqrL6MgTb6cfAjep/NdaGfHnwGUDWrc0Ol2beIu5Ikz0SzcAW46F2HY7/GglRUtBXUCCw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:12:56.869976Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.24800","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:62aa08da20369c047b311f6060e50ba84b333c3080b6f9dd14fd9d35a2069705","sha256:260ffb6b2059e21a1999f0b2cbc320d508b055cecd4641a3e3154e75fcbaebdd"],"state_sha256":"39876a14c8e4c88c136a6744d8ae1811147a20145d49178642af9d79b4588247"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XEfM/D9HEAUFsShRRBdUb+Fch9ofIdgqlRsC4gua0+xNO5hWR/+RUH51znu3NiOT5Aao2Zi5LWKTQ69526KrDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T01:15:26.746830Z","bundle_sha256":"2313075a9f529967b00c5f5821f6c9a3af43538000acd3c587fd40f0f21c65ca"}}