{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2020:ZCOVQGTMQZM3L2AFPUAXMDS6HA","short_pith_number":"pith:ZCOVQGTM","canonical_record":{"source":{"id":"2010.11071","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2020-10-21T15:22:27Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"a846c6f5642f5bf821833d67c701d2afe2a8e696894a16f23417436d10c09abb","abstract_canon_sha256":"bdf51e040e9915b0af72425164b0b103d743f029544535d2c8fd4b24b37ff8ff"},"schema_version":"1.0"},"canonical_sha256":"c89d581a6c8659b5e8057d01760e5e381f9b477425e7f7d594c190c6dd6b3041","source":{"kind":"arxiv","id":"2010.11071","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2010.11071","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"arxiv_version","alias_value":"2010.11071v1","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.11071","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_12","alias_value":"ZCOVQGTMQZM3","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_16","alias_value":"ZCOVQGTMQZM3L2AF","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_8","alias_value":"ZCOVQGTM","created_at":"2026-07-05T01:44:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2020:ZCOVQGTMQZM3L2AFPUAXMDS6HA","target":"record","payload":{"canonical_record":{"source":{"id":"2010.11071","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2020-10-21T15:22:27Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"a846c6f5642f5bf821833d67c701d2afe2a8e696894a16f23417436d10c09abb","abstract_canon_sha256":"bdf51e040e9915b0af72425164b0b103d743f029544535d2c8fd4b24b37ff8ff"},"schema_version":"1.0"},"canonical_sha256":"c89d581a6c8659b5e8057d01760e5e381f9b477425e7f7d594c190c6dd6b3041","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:44:58.976630Z","signature_b64":"Q7m6T0GOaWsVpXJWCSl8TIBNIatrlPwj959TqgxLdqJXLoOSiIroxANG/jagiUX81TJTBYXY0y//nJb9Nby1Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c89d581a6c8659b5e8057d01760e5e381f9b477425e7f7d594c190c6dd6b3041","last_reissued_at":"2026-07-05T01:44:58.976157Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:44:58.976157Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2010.11071","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":"2026-07-05T01:44:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7pc+Xoex96oBCyF2kdr8kAgQmNEkKlM8/uyO3Pbh5PMcXhQqSjopvvTju/Dl3k0oRZlyVBxJQz3MbwLt/vR8CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T09:57:31.391197Z"},"content_sha256":"50b35a569e4ae9d1a8788f958609c24587cf5c049278a74c867d9f9a1a2aff34","schema_version":"1.0","event_id":"sha256:50b35a569e4ae9d1a8788f958609c24587cf5c049278a74c867d9f9a1a2aff34"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2020:ZCOVQGTMQZM3L2AFPUAXMDS6HA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Extreme renormalisations of dimer eigenmodes by strong light-matter coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Carsten Rockstuhl, Charles A. Downing, Magdalena Stobi\\'nska, Taavi Rep\\\"an, Thomas J. Sturges","submitted_at":"2020-10-21T15:22:27Z","abstract_excerpt":"We explore by theoretical means an extreme renormalisation of the eigenmodes of a dimer of dipolar meta-atoms due to strong light-matter interactions. Firstly, by tuning the height of an enclosing photonic cavity, we can lower the energy level of the symmetric `bright' mode underneath that of the anti-symmetric `dark' mode. This is possible due to the polaritonic nature of the symmetric mode, that shares simultaneously its excitation with the cavity and the dimer. For a heterogeneous dimer, we show that the polariton modes can be smoothly tuned from symmetric to anti-symmetric, resulting in a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.11071","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/2010.11071/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":"2026-07-05T01:44:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I7RB2y4Su3KvPZ0uInGeWKtm/npWYmJw4nn1nRmHRz7OOGiYKSoGMTjWTpBpeVEkS3nHlDGZpqEjK32kAE36Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T09:57:31.391587Z"},"content_sha256":"39be7436686f6241a53133e549af115b8382800dd2427651126e4aeea4409e74","schema_version":"1.0","event_id":"sha256:39be7436686f6241a53133e549af115b8382800dd2427651126e4aeea4409e74"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/bundle.json","state_url":"https://pith.science/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/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":"2026-07-14T09:57:31Z","links":{"resolver":"https://pith.science/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA","bundle":"https://pith.science/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/bundle.json","state":"https://pith.science/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZCOVQGTMQZM3L2AFPUAXMDS6HA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:ZCOVQGTMQZM3L2AFPUAXMDS6HA","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":"bdf51e040e9915b0af72425164b0b103d743f029544535d2c8fd4b24b37ff8ff","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2020-10-21T15:22:27Z","title_canon_sha256":"a846c6f5642f5bf821833d67c701d2afe2a8e696894a16f23417436d10c09abb"},"schema_version":"1.0","source":{"id":"2010.11071","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2010.11071","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"arxiv_version","alias_value":"2010.11071v1","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.11071","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_12","alias_value":"ZCOVQGTMQZM3","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_16","alias_value":"ZCOVQGTMQZM3L2AF","created_at":"2026-07-05T01:44:58Z"},{"alias_kind":"pith_short_8","alias_value":"ZCOVQGTM","created_at":"2026-07-05T01:44:58Z"}],"graph_snapshots":[{"event_id":"sha256:39be7436686f6241a53133e549af115b8382800dd2427651126e4aeea4409e74","target":"graph","created_at":"2026-07-05T01:44:58Z","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/2010.11071/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We explore by theoretical means an extreme renormalisation of the eigenmodes of a dimer of dipolar meta-atoms due to strong light-matter interactions. Firstly, by tuning the height of an enclosing photonic cavity, we can lower the energy level of the symmetric `bright' mode underneath that of the anti-symmetric `dark' mode. This is possible due to the polaritonic nature of the symmetric mode, that shares simultaneously its excitation with the cavity and the dimer. For a heterogeneous dimer, we show that the polariton modes can be smoothly tuned from symmetric to anti-symmetric, resulting in a ","authors_text":"Carsten Rockstuhl, Charles A. Downing, Magdalena Stobi\\'nska, Taavi Rep\\\"an, Thomas J. Sturges","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2020-10-21T15:22:27Z","title":"Extreme renormalisations of dimer eigenmodes by strong light-matter coupling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.11071","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":"sha256:50b35a569e4ae9d1a8788f958609c24587cf5c049278a74c867d9f9a1a2aff34","target":"record","created_at":"2026-07-05T01:44:58Z","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":"bdf51e040e9915b0af72425164b0b103d743f029544535d2c8fd4b24b37ff8ff","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2020-10-21T15:22:27Z","title_canon_sha256":"a846c6f5642f5bf821833d67c701d2afe2a8e696894a16f23417436d10c09abb"},"schema_version":"1.0","source":{"id":"2010.11071","kind":"arxiv","version":1}},"canonical_sha256":"c89d581a6c8659b5e8057d01760e5e381f9b477425e7f7d594c190c6dd6b3041","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c89d581a6c8659b5e8057d01760e5e381f9b477425e7f7d594c190c6dd6b3041","first_computed_at":"2026-07-05T01:44:58.976157Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:44:58.976157Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q7m6T0GOaWsVpXJWCSl8TIBNIatrlPwj959TqgxLdqJXLoOSiIroxANG/jagiUX81TJTBYXY0y//nJb9Nby1Cg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:44:58.976630Z","signed_message":"canonical_sha256_bytes"},"source_id":"2010.11071","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:50b35a569e4ae9d1a8788f958609c24587cf5c049278a74c867d9f9a1a2aff34","sha256:39be7436686f6241a53133e549af115b8382800dd2427651126e4aeea4409e74"],"state_sha256":"78a7763f62942034c1e27d309f054a8a4b06e0374914e39cba122d135fffa557"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mMUpARYWB1v7Xv8ta2fT/qcVK3eV65Te1sWyRCZde7nC1BL9ZMGGDiYxjGY9X+SD5YWaPhGfIW4/Y7n8gENoDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-14T09:57:31.393758Z","bundle_sha256":"5c68bbb34c18dee63391db77624658b726db4b5a37daaabfcca3f0de39a37706"}}