{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:STBD7XQLAFAG75KZG2NPJNC5FV","short_pith_number":"pith:STBD7XQL","canonical_record":{"source":{"id":"1411.5561","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-20T14:40:47Z","cross_cats_sorted":[],"title_canon_sha256":"fd01aa751d150196d07b7b9a9f38df910a70787b826f2126624679533691a25e","abstract_canon_sha256":"c8ddbaccf5595981b2bcfe1fb3b79b2f5b27d9b0f38773651367f1835279cc41"},"schema_version":"1.0"},"canonical_sha256":"94c23fde0b01406ff559369af4b45d2d65b524e4e928e666b3e75c759185fd63","source":{"kind":"arxiv","id":"1411.5561","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.5561","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"arxiv_version","alias_value":"1411.5561v2","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.5561","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"pith_short_12","alias_value":"STBD7XQLAFAG","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"STBD7XQLAFAG75KZ","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"STBD7XQL","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:STBD7XQLAFAG75KZG2NPJNC5FV","target":"record","payload":{"canonical_record":{"source":{"id":"1411.5561","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-20T14:40:47Z","cross_cats_sorted":[],"title_canon_sha256":"fd01aa751d150196d07b7b9a9f38df910a70787b826f2126624679533691a25e","abstract_canon_sha256":"c8ddbaccf5595981b2bcfe1fb3b79b2f5b27d9b0f38773651367f1835279cc41"},"schema_version":"1.0"},"canonical_sha256":"94c23fde0b01406ff559369af4b45d2d65b524e4e928e666b3e75c759185fd63","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:51.669614Z","signature_b64":"4Fcbpv3xl53JHe6u1vz5VDfUrfwB/S6v418Q2e8ZtjoQ15eYYMuIEmsG9R1NdnY9B1Vxvz2W2qP/h9+slBRSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94c23fde0b01406ff559369af4b45d2d65b524e4e928e666b3e75c759185fd63","last_reissued_at":"2026-05-18T02:17:51.668836Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:51.668836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.5561","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":"2026-05-18T02:17:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RTudpAQQjTmJ0Gcri1Vit9cenDxdaGk+Joyh+Q041wskxDKYL4ToSLjmDy15Dze6sOcqfMr9ZRyNYV6h2t0ZCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:10:39.798305Z"},"content_sha256":"06791d9f2170f24ff4b0029bd2cdc60a185fe501140217fec381430d072c7991","schema_version":"1.0","event_id":"sha256:06791d9f2170f24ff4b0029bd2cdc60a185fe501140217fec381430d072c7991"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:STBD7XQLAFAG75KZG2NPJNC5FV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Linear and Non-linear Rabi Oscillations of a Two-Level System Resonantly Coupled to an Anderson-Localized Mode","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Christian Vanneste, Nicolas Bachelard, Patrick Sebbah, R\\'emi Carminati","submitted_at":"2014-11-20T14:40:47Z","abstract_excerpt":"We use time-domain numerical simulations of a two-dimensional (2D) scattering system to study the interaction of a collection of emitters resonantly coupled to an Anderson-localized mode. For a small electric field intensity, we observe the strong coupling between the emitters and the mode, which is characterized by linear Rabi oscillations. Remarkably, a larger intensity induces non-linear interaction between the emitters and the mode, referred to as the dynamical Stark effect, resulting in non-linear Rabi oscillations. The transition between both regimes is observed and an analytical model i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.5561","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":"2026-05-18T02:17:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SuH0+NNGmVKDVfF57a7GRlNckYoELrol9EZoYta3Pme3pgMW73yKueZNgeRZhI5A9XltlGS4VlEhVZvHkGauAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:10:39.798980Z"},"content_sha256":"99eb4b69f4219ae060026d5fc915d470d7b93e34e05c4f74fb3a7b68095f14ad","schema_version":"1.0","event_id":"sha256:99eb4b69f4219ae060026d5fc915d470d7b93e34e05c4f74fb3a7b68095f14ad"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/STBD7XQLAFAG75KZG2NPJNC5FV/bundle.json","state_url":"https://pith.science/pith/STBD7XQLAFAG75KZG2NPJNC5FV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/STBD7XQLAFAG75KZG2NPJNC5FV/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":"2026-05-30T13:10:39Z","links":{"resolver":"https://pith.science/pith/STBD7XQLAFAG75KZG2NPJNC5FV","bundle":"https://pith.science/pith/STBD7XQLAFAG75KZG2NPJNC5FV/bundle.json","state":"https://pith.science/pith/STBD7XQLAFAG75KZG2NPJNC5FV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/STBD7XQLAFAG75KZG2NPJNC5FV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:STBD7XQLAFAG75KZG2NPJNC5FV","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":"c8ddbaccf5595981b2bcfe1fb3b79b2f5b27d9b0f38773651367f1835279cc41","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-20T14:40:47Z","title_canon_sha256":"fd01aa751d150196d07b7b9a9f38df910a70787b826f2126624679533691a25e"},"schema_version":"1.0","source":{"id":"1411.5561","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.5561","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"arxiv_version","alias_value":"1411.5561v2","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.5561","created_at":"2026-05-18T02:17:51Z"},{"alias_kind":"pith_short_12","alias_value":"STBD7XQLAFAG","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"STBD7XQLAFAG75KZ","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"STBD7XQL","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:99eb4b69f4219ae060026d5fc915d470d7b93e34e05c4f74fb3a7b68095f14ad","target":"graph","created_at":"2026-05-18T02:17:51Z","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 use time-domain numerical simulations of a two-dimensional (2D) scattering system to study the interaction of a collection of emitters resonantly coupled to an Anderson-localized mode. For a small electric field intensity, we observe the strong coupling between the emitters and the mode, which is characterized by linear Rabi oscillations. Remarkably, a larger intensity induces non-linear interaction between the emitters and the mode, referred to as the dynamical Stark effect, resulting in non-linear Rabi oscillations. The transition between both regimes is observed and an analytical model i","authors_text":"Christian Vanneste, Nicolas Bachelard, Patrick Sebbah, R\\'emi Carminati","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-20T14:40:47Z","title":"Linear and Non-linear Rabi Oscillations of a Two-Level System Resonantly Coupled to an Anderson-Localized Mode"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.5561","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":"sha256:06791d9f2170f24ff4b0029bd2cdc60a185fe501140217fec381430d072c7991","target":"record","created_at":"2026-05-18T02:17:51Z","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":"c8ddbaccf5595981b2bcfe1fb3b79b2f5b27d9b0f38773651367f1835279cc41","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-11-20T14:40:47Z","title_canon_sha256":"fd01aa751d150196d07b7b9a9f38df910a70787b826f2126624679533691a25e"},"schema_version":"1.0","source":{"id":"1411.5561","kind":"arxiv","version":2}},"canonical_sha256":"94c23fde0b01406ff559369af4b45d2d65b524e4e928e666b3e75c759185fd63","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"94c23fde0b01406ff559369af4b45d2d65b524e4e928e666b3e75c759185fd63","first_computed_at":"2026-05-18T02:17:51.668836Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:17:51.668836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4Fcbpv3xl53JHe6u1vz5VDfUrfwB/S6v418Q2e8ZtjoQ15eYYMuIEmsG9R1NdnY9B1Vxvz2W2qP/h9+slBRSCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:17:51.669614Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.5561","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:06791d9f2170f24ff4b0029bd2cdc60a185fe501140217fec381430d072c7991","sha256:99eb4b69f4219ae060026d5fc915d470d7b93e34e05c4f74fb3a7b68095f14ad"],"state_sha256":"c92421b831dff416fee36f4bb12f4a8a7e053ac04c0c7d8339437b6f6b0bfde4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aJscwrMfPRJyDH18SGwbenFEU6KeJYPDbnGigvZRAy6fpcQx8uI5hG0Eth6RNMSUr28reyJGOUVX1BGEDUE8DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T13:10:39.803604Z","bundle_sha256":"4e99eb0bc3bc0d2d3947b423b04f92efb27c794ed8a1f9bbcdfb5130d6f07b75"}}