{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:VXXVKY3VHEQ5DX5DIWVI4GOHC6","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":"1f70077b74c6c5d0f63cfc94b8d95e1d4fe49b9013e30b12ac2f1eb00f0af0a5","cross_cats_sorted":["physics.app-ph","physics.optics"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"quant-ph","submitted_at":"2023-11-13T05:19:59Z","title_canon_sha256":"eb5c64c1e81c757dff69d00d690d05aaef6533d62f1ce66abd12e76ccefe5bf5"},"schema_version":"1.0","source":{"id":"2311.07083","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2311.07083","created_at":"2026-07-05T08:20:08Z"},{"alias_kind":"arxiv_version","alias_value":"2311.07083v1","created_at":"2026-07-05T08:20:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.07083","created_at":"2026-07-05T08:20:08Z"},{"alias_kind":"pith_short_12","alias_value":"VXXVKY3VHEQ5","created_at":"2026-07-05T08:20:08Z"},{"alias_kind":"pith_short_16","alias_value":"VXXVKY3VHEQ5DX5D","created_at":"2026-07-05T08:20:08Z"},{"alias_kind":"pith_short_8","alias_value":"VXXVKY3V","created_at":"2026-07-05T08:20:08Z"}],"graph_snapshots":[{"event_id":"sha256:d60c0b855bca232dcb66a1c632c623953cab6697f44617d49bcc6ffb1585a68d","target":"graph","created_at":"2026-07-05T08:20:08Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2311.07083/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We exploit InSb's magnetic-induced optical properties to propose THz sub-wavelength antenna designs that actively tune the radiative decay rates of dipole emitters at their proximity. The proposed designs include a spherical InSb antenna and a cylindrical Si-InSb hybrid antenna that demonstrate distinct behaviors; the former dramatically enhances both radiative and non-radiative decay rates in the epsilon-near-zero region due to the dominant contribution of the Zeeman splitting electric octupole mode. The latter realizes significant radiative decay rate enhancement via magnetic octupole mode, ","authors_text":"Amirreza Ahmadnejad, Carsten Rockstuhl, Ehsan Mobini, Ksenia Dolgaleva, Mohamadreza Mohamadpour, Rasoul Alaee, Robert W. Boyd, Sina Aghili","cross_cats":["physics.app-ph","physics.optics"],"headline":"","license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"quant-ph","submitted_at":"2023-11-13T05:19:59Z","title":"Dynamic Control of Spontaneous Emission Using Magnetized InSb Higher-Order-Mode Antennas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.07083","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":"sha256:0e01ace45f6b038bd09f92164a463970aaccbe29ce991c0ea1464361aed97271","target":"record","created_at":"2026-07-05T08:20:08Z","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":"1f70077b74c6c5d0f63cfc94b8d95e1d4fe49b9013e30b12ac2f1eb00f0af0a5","cross_cats_sorted":["physics.app-ph","physics.optics"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"quant-ph","submitted_at":"2023-11-13T05:19:59Z","title_canon_sha256":"eb5c64c1e81c757dff69d00d690d05aaef6533d62f1ce66abd12e76ccefe5bf5"},"schema_version":"1.0","source":{"id":"2311.07083","kind":"arxiv","version":1}},"canonical_sha256":"adef5563753921d1dfa345aa8e19c71788542e462e35777aa636616cce5647a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"adef5563753921d1dfa345aa8e19c71788542e462e35777aa636616cce5647a2","first_computed_at":"2026-07-05T08:20:08.582504Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:20:08.582504Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EZ6ZLoVmNfxd8BOraUhjQ9Ul36LaLsKQGjznh/bbu5lftBcZXr0kKOm2ersEfDu2tjRyohSwN+XrqZptllO8CQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:20:08.582903Z","signed_message":"canonical_sha256_bytes"},"source_id":"2311.07083","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0e01ace45f6b038bd09f92164a463970aaccbe29ce991c0ea1464361aed97271","sha256:d60c0b855bca232dcb66a1c632c623953cab6697f44617d49bcc6ffb1585a68d"],"state_sha256":"20cfb80aafd6d84daa5511cd51a3f97059820a7b194c6c81c8240399d5799670"}