{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:RXXFJYWRVCWXA42DZI3FAAZSTO","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":"9ee3914f4d063b136b526efa87ef708eb855d45fd0ae2ab4d8cf1c4108b592f4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-12-12T23:38:44Z","title_canon_sha256":"7a6c3859e96b6449c36d4c0ee2fe568d369390a592c285a74a991fa55b75fe34"},"schema_version":"1.0","source":{"id":"1512.03977","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.03977","created_at":"2026-05-18T01:18:30Z"},{"alias_kind":"arxiv_version","alias_value":"1512.03977v1","created_at":"2026-05-18T01:18:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.03977","created_at":"2026-05-18T01:18:30Z"},{"alias_kind":"pith_short_12","alias_value":"RXXFJYWRVCWX","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"RXXFJYWRVCWXA42D","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"RXXFJYWR","created_at":"2026-05-18T12:29:39Z"}],"graph_snapshots":[{"event_id":"sha256:49de8539b3daee4d81b87b68bcda78da3cc328368e3b338ae0515710048b4a40","target":"graph","created_at":"2026-05-18T01:18:30Z","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":"The concept of high refractive index subwavelength dielectric nanoresonators, supporting electric and magnetic optical resonances, is a promising platform for waveguiding, sensing, and nonlinear nanophotonic devices. However, high concentration of defects in the nanoresonators diminishes their resonant properties, which are crucially dependent on their internal losses. Therefore, it seems to be inevitable to use initially crystalline materials for fabrication of the nanoresonators. Here, we show that the fabrication of crystalline (low-loss) resonant silicon nanoparticles by femtosecond laser ","authors_text":"A. A. Sitnikova, A.E. Krasnok, A.K. Samusev, A.S. Gudovskikh, I.S. Mukhin, P.A. Belov, P.A. Dmitriev, S.V. Makarov, V.A. Milichko","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-12-12T23:38:44Z","title":"Laser fabrication of crystalline silicon nanoresonators from an amorphous film for low-loss all-dielectric nanophotonics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.03977","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":"sha256:3970abd10a58f636dc857ff944ef01a0b53bc32892c269bfccea6744a24c4152","target":"record","created_at":"2026-05-18T01:18:30Z","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":"9ee3914f4d063b136b526efa87ef708eb855d45fd0ae2ab4d8cf1c4108b592f4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2015-12-12T23:38:44Z","title_canon_sha256":"7a6c3859e96b6449c36d4c0ee2fe568d369390a592c285a74a991fa55b75fe34"},"schema_version":"1.0","source":{"id":"1512.03977","kind":"arxiv","version":1}},"canonical_sha256":"8dee54e2d1a8ad707343ca365003329bbd2f64210ee3009e2505f54cc1595b4e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8dee54e2d1a8ad707343ca365003329bbd2f64210ee3009e2505f54cc1595b4e","first_computed_at":"2026-05-18T01:18:30.170485Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:18:30.170485Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vHLXfUyxd8q8PtOTPAmPMtU7hUhVy9OcZyKvhftLjLKFPS5A6iXM4w8aM5i5pcMhdU89oWbjMnIe5LumfzI0DA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:18:30.171005Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.03977","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3970abd10a58f636dc857ff944ef01a0b53bc32892c269bfccea6744a24c4152","sha256:49de8539b3daee4d81b87b68bcda78da3cc328368e3b338ae0515710048b4a40"],"state_sha256":"707f9e3bfdfe847611e276b1e0547b9403476acb31add1dbcefad7dd402e4f2d"}