{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:UL2S37OCVLRJDNVNVMXAMJQYQF","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":"bb65c488da6c370dbd960b5c0c9dad3aba3f26dce0fb2c1688640c8676d35faa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-06-02T16:41:25Z","title_canon_sha256":"e6a751e524b33b681caf89e846bc4d3bf51e1d249cbd19b8fd1a7050d91b9f12"},"schema_version":"1.0","source":{"id":"1606.02163","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.02163","created_at":"2026-05-18T00:50:29Z"},{"alias_kind":"arxiv_version","alias_value":"1606.02163v1","created_at":"2026-05-18T00:50:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.02163","created_at":"2026-05-18T00:50:29Z"},{"alias_kind":"pith_short_12","alias_value":"UL2S37OCVLRJ","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_16","alias_value":"UL2S37OCVLRJDNVN","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_8","alias_value":"UL2S37OC","created_at":"2026-05-18T12:30:46Z"}],"graph_snapshots":[{"event_id":"sha256:a8acf8aa3973683450b3a49a2d8d447032074d864a0f0967a47d5a1a9d90b673","target":"graph","created_at":"2026-05-18T00:50:29Z","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":"Electromagnetic scattering in accelerating reference frames inspires a variety of phenomena, requiring employment of general relativity for their description. While the quasi-stationary field analysis could be applied to slowly-accelerating bodies as a first-order approximation, the scattering problem remains fundamentally nonlinear in boundary conditions, giving rise to multiple frequency generation (micro-Doppler shifts). Here a frequency comb, generated by an axially rotating subwavelength (cm-range) wire and split ring resonator (SRR), is analyzed theoretically and observed experimentally ","authors_text":"Dmitrii Filonov, Pavel Ginzburg, Vitali Kozlov, Yefim Yankelevich","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-06-02T16:41:25Z","title":"Micro-Doppler Frequency Comb Generation by Axially Rotating Scatterers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.02163","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:e92020f1cac366976dddd67eb6dc17cef8d6ff2b7182062c7ddb0494e128e26a","target":"record","created_at":"2026-05-18T00:50:29Z","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":"bb65c488da6c370dbd960b5c0c9dad3aba3f26dce0fb2c1688640c8676d35faa","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-06-02T16:41:25Z","title_canon_sha256":"e6a751e524b33b681caf89e846bc4d3bf51e1d249cbd19b8fd1a7050d91b9f12"},"schema_version":"1.0","source":{"id":"1606.02163","kind":"arxiv","version":1}},"canonical_sha256":"a2f52dfdc2aae291b6adab2e06261881582e5fe4a44a670fa065804573a29c7f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a2f52dfdc2aae291b6adab2e06261881582e5fe4a44a670fa065804573a29c7f","first_computed_at":"2026-05-18T00:50:29.510592Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:50:29.510592Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NIgCekZ67t01LvEOUBkIs3Trr5lexsD1HGpIy1qj/aVI5gKJZAT7SZFA8E4Iog9iXs+TwCHkksAGYWvavutTAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:50:29.511258Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.02163","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e92020f1cac366976dddd67eb6dc17cef8d6ff2b7182062c7ddb0494e128e26a","sha256:a8acf8aa3973683450b3a49a2d8d447032074d864a0f0967a47d5a1a9d90b673"],"state_sha256":"d89618171d78246611d59d8df3ff104d149248acc64cb720adcdd70131dc549c"}