{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:RHUZXJKJABA4NVZPV5L4WAPGJ5","short_pith_number":"pith:RHUZXJKJ","canonical_record":{"source":{"id":"1710.03685","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-10-02T07:34:06Z","cross_cats_sorted":["physics.app-ph","physics.optics"],"title_canon_sha256":"6392b3175ad2c2d8221a3019a362745401b6220b525234b26aa0a312e7c13c2d","abstract_canon_sha256":"461ee0feb7d230620d7224da0ab2fd182d0d51dadbef81ebeebbf90ecd1457ec"},"schema_version":"1.0"},"canonical_sha256":"89e99ba5490041c6d72faf57cb01e64f43164b0ddb02116f3f3bc1cd06332076","source":{"kind":"arxiv","id":"1710.03685","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.03685","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"arxiv_version","alias_value":"1710.03685v2","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.03685","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"pith_short_12","alias_value":"RHUZXJKJABA4","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RHUZXJKJABA4NVZP","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RHUZXJKJ","created_at":"2026-05-18T12:31:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:RHUZXJKJABA4NVZPV5L4WAPGJ5","target":"record","payload":{"canonical_record":{"source":{"id":"1710.03685","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-10-02T07:34:06Z","cross_cats_sorted":["physics.app-ph","physics.optics"],"title_canon_sha256":"6392b3175ad2c2d8221a3019a362745401b6220b525234b26aa0a312e7c13c2d","abstract_canon_sha256":"461ee0feb7d230620d7224da0ab2fd182d0d51dadbef81ebeebbf90ecd1457ec"},"schema_version":"1.0"},"canonical_sha256":"89e99ba5490041c6d72faf57cb01e64f43164b0ddb02116f3f3bc1cd06332076","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:30.605405Z","signature_b64":"UvraJTjBd+xgl6VQo0VHQOa3FjhydgosMxOGoJ/7mQ47BuUrS02YzIhN0fdwMrBchqblmOXGG/exRrcmINaBBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89e99ba5490041c6d72faf57cb01e64f43164b0ddb02116f3f3bc1cd06332076","last_reissued_at":"2026-05-18T00:24:30.604953Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:30.604953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.03685","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":"2026-05-18T00:24:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mV6ArCw+N6HiBjt3SvNSiYP6oMyidH0U3hk99IT9WpbQbqU0tT08t9G5tGdAVeDjWarZf6/v4+FgNIrwFfUfAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T15:03:41.050558Z"},"content_sha256":"356766e0f072837cb1f53048fafcbe71ac752ea80fdd368f8717ab4471d6df65","schema_version":"1.0","event_id":"sha256:356766e0f072837cb1f53048fafcbe71ac752ea80fdd368f8717ab4471d6df65"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:RHUZXJKJABA4NVZPV5L4WAPGJ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High-quality trapped modes in all-dielectric metamaterials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.app-ph","physics.optics"],"primary_cat":"physics.class-ph","authors_text":"Anton S. Kupriianov, Hai Wang, Hong-Bo Sun, Kateryna L. Domina, Su Xu, Vladimir R. Tuz, Vyacheslav V. Khardikov","submitted_at":"2017-10-02T07:34:06Z","abstract_excerpt":"A planar all-dielectric metamaterial made of a double-periodic lattice whose unit cell consists of a single subwavelength dielectric particle having the form of a disk possessing a penetrating hole is considered. The resonant states in the transmitted spectra of the metamaterial are identified considering modes inherent to the individual cylindrical dielectric resonator. A correlation between the asymmetry in particle's geometry, which arises from the off-centered displacement of the hole, and formation of the Mie-type and trapped modes is established. The advantages of using a coaxial-sector "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.03685","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":"2026-05-18T00:24:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fo2teWhWICPEfwIQbW/dp1ea6TJ+7p3iLpH73+woqYT7zmB0Pn2EOTlEi+ZzCvqzMis/nhJe+tMKEtYWEICZBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T15:03:41.050931Z"},"content_sha256":"39cbf70ff39d1602d771035fc58000fac695b509489f2b216a1956680d5149d1","schema_version":"1.0","event_id":"sha256:39cbf70ff39d1602d771035fc58000fac695b509489f2b216a1956680d5149d1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/bundle.json","state_url":"https://pith.science/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/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":"2026-05-29T15:03:41Z","links":{"resolver":"https://pith.science/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5","bundle":"https://pith.science/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/bundle.json","state":"https://pith.science/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RHUZXJKJABA4NVZPV5L4WAPGJ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:RHUZXJKJABA4NVZPV5L4WAPGJ5","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":"461ee0feb7d230620d7224da0ab2fd182d0d51dadbef81ebeebbf90ecd1457ec","cross_cats_sorted":["physics.app-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-10-02T07:34:06Z","title_canon_sha256":"6392b3175ad2c2d8221a3019a362745401b6220b525234b26aa0a312e7c13c2d"},"schema_version":"1.0","source":{"id":"1710.03685","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.03685","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"arxiv_version","alias_value":"1710.03685v2","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.03685","created_at":"2026-05-18T00:24:30Z"},{"alias_kind":"pith_short_12","alias_value":"RHUZXJKJABA4","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RHUZXJKJABA4NVZP","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RHUZXJKJ","created_at":"2026-05-18T12:31:39Z"}],"graph_snapshots":[{"event_id":"sha256:39cbf70ff39d1602d771035fc58000fac695b509489f2b216a1956680d5149d1","target":"graph","created_at":"2026-05-18T00:24:30Z","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":"A planar all-dielectric metamaterial made of a double-periodic lattice whose unit cell consists of a single subwavelength dielectric particle having the form of a disk possessing a penetrating hole is considered. The resonant states in the transmitted spectra of the metamaterial are identified considering modes inherent to the individual cylindrical dielectric resonator. A correlation between the asymmetry in particle's geometry, which arises from the off-centered displacement of the hole, and formation of the Mie-type and trapped modes is established. The advantages of using a coaxial-sector ","authors_text":"Anton S. Kupriianov, Hai Wang, Hong-Bo Sun, Kateryna L. Domina, Su Xu, Vladimir R. Tuz, Vyacheslav V. Khardikov","cross_cats":["physics.app-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-10-02T07:34:06Z","title":"High-quality trapped modes in all-dielectric metamaterials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.03685","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":"sha256:356766e0f072837cb1f53048fafcbe71ac752ea80fdd368f8717ab4471d6df65","target":"record","created_at":"2026-05-18T00:24:30Z","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":"461ee0feb7d230620d7224da0ab2fd182d0d51dadbef81ebeebbf90ecd1457ec","cross_cats_sorted":["physics.app-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-10-02T07:34:06Z","title_canon_sha256":"6392b3175ad2c2d8221a3019a362745401b6220b525234b26aa0a312e7c13c2d"},"schema_version":"1.0","source":{"id":"1710.03685","kind":"arxiv","version":2}},"canonical_sha256":"89e99ba5490041c6d72faf57cb01e64f43164b0ddb02116f3f3bc1cd06332076","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89e99ba5490041c6d72faf57cb01e64f43164b0ddb02116f3f3bc1cd06332076","first_computed_at":"2026-05-18T00:24:30.604953Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:30.604953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UvraJTjBd+xgl6VQo0VHQOa3FjhydgosMxOGoJ/7mQ47BuUrS02YzIhN0fdwMrBchqblmOXGG/exRrcmINaBBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:30.605405Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.03685","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:356766e0f072837cb1f53048fafcbe71ac752ea80fdd368f8717ab4471d6df65","sha256:39cbf70ff39d1602d771035fc58000fac695b509489f2b216a1956680d5149d1"],"state_sha256":"9503013fd9e48aa6201cf2eeb7d01cbb5a141b1e0e192e1d62bab98ee6d4ed0d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gsQP3MHiIZwADsSqOivpE0jYICg3K/kpKexH02WZWgfXKY58KaeDVfYKAyaZiaUm8RYdmq/1G5Mpfy9ROl3FCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T15:03:41.054301Z","bundle_sha256":"b8065fd9dbd99b6593cb9d78e77e8f3e8cc4b893c09c8e78e0d51b8dbd5d8d53"}}