{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:YSRT3Z23RYUZTWCEB7VFM6Q5SG","short_pith_number":"pith:YSRT3Z23","canonical_record":{"source":{"id":"1707.00864","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-04T09:06:37Z","cross_cats_sorted":[],"title_canon_sha256":"bdd5f9650061af896d2ef872a628aba40788d84d26ab6f24a36338ac63b64325","abstract_canon_sha256":"5af49d02242e95c5e93865a2564ca953b06398ac5db8dc58246d99f75d2a4d33"},"schema_version":"1.0"},"canonical_sha256":"c4a33de75b8e2999d8440fea567a1d91bc1882228bdc4f9f6f4bfcbc871a6c60","source":{"kind":"arxiv","id":"1707.00864","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.00864","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"arxiv_version","alias_value":"1707.00864v1","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.00864","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"pith_short_12","alias_value":"YSRT3Z23RYUZ","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YSRT3Z23RYUZTWCE","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YSRT3Z23","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:YSRT3Z23RYUZTWCEB7VFM6Q5SG","target":"record","payload":{"canonical_record":{"source":{"id":"1707.00864","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-04T09:06:37Z","cross_cats_sorted":[],"title_canon_sha256":"bdd5f9650061af896d2ef872a628aba40788d84d26ab6f24a36338ac63b64325","abstract_canon_sha256":"5af49d02242e95c5e93865a2564ca953b06398ac5db8dc58246d99f75d2a4d33"},"schema_version":"1.0"},"canonical_sha256":"c4a33de75b8e2999d8440fea567a1d91bc1882228bdc4f9f6f4bfcbc871a6c60","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:56.791615Z","signature_b64":"7Sm/3jU8Z1m7xBeYVDb5OzoC4Pw7S++0XNheNQUq7Wt9vrsevodGb+jwFwaP0rIKUZDZOqI+Lia2dNpGhoARBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c4a33de75b8e2999d8440fea567a1d91bc1882228bdc4f9f6f4bfcbc871a6c60","last_reissued_at":"2026-05-18T00:40:56.791028Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:56.791028Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.00864","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":"2026-05-18T00:40:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XK3BZpOrQ/kSW9cyl2Ie8G9etfBQZPnJGW1RVS9qQmMYjP3QG6iPoNSilzfj7M9LPd04nXrXD4dJng1VKYhrAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:33:23.192349Z"},"content_sha256":"4a0b6f41de75ed8c8f08fc06a4eb432ecc373976aae967a7ae750b97c45504cd","schema_version":"1.0","event_id":"sha256:4a0b6f41de75ed8c8f08fc06a4eb432ecc373976aae967a7ae750b97c45504cd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:YSRT3Z23RYUZTWCEB7VFM6Q5SG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tuning of bound states in the continuum by waveguide rotation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Alina A. Lyapina, Almas F. Sadreev, Artem S. Pilipchuk","submitted_at":"2017-07-04T09:06:37Z","abstract_excerpt":"We consider acoustic wave transmission in non axisymmetric waveguide which consists of cylindrical resonator and two semi-infinite cylindrical waveguides whose axes are shifted relative to the resonator axis and each other by azimuthal angle $\\Delta\\phi$. We show that for rotation of one of attached waveguides the coupling matrix elements of the eigenmodes of resonator classified by the integer $m$ and propagating mode of the waveguide acquire phase factor $e^{im\\Delta\\phi}$. That crucially effect Fano resonances and creates an analog of faucet opening and closing wave flux under rotation of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.00864","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":""},"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":"2026-05-18T00:40:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mQ+a9xmKu0jpThbD5OOoJFc4UaSIZ0pGHe3MEXTMd+R0GaBwTZ6Fvu36oYOh3NFOOLoauH7g21HqLRFxD8dZCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:33:23.193055Z"},"content_sha256":"0dd99bace5d68b2a65af43b569d8f3a3456cfe37152586a9bc215cc1d17f2b63","schema_version":"1.0","event_id":"sha256:0dd99bace5d68b2a65af43b569d8f3a3456cfe37152586a9bc215cc1d17f2b63"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/bundle.json","state_url":"https://pith.science/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/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":"2026-06-09T18:33:23Z","links":{"resolver":"https://pith.science/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG","bundle":"https://pith.science/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/bundle.json","state":"https://pith.science/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YSRT3Z23RYUZTWCEB7VFM6Q5SG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:YSRT3Z23RYUZTWCEB7VFM6Q5SG","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":"5af49d02242e95c5e93865a2564ca953b06398ac5db8dc58246d99f75d2a4d33","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-04T09:06:37Z","title_canon_sha256":"bdd5f9650061af896d2ef872a628aba40788d84d26ab6f24a36338ac63b64325"},"schema_version":"1.0","source":{"id":"1707.00864","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.00864","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"arxiv_version","alias_value":"1707.00864v1","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.00864","created_at":"2026-05-18T00:40:56Z"},{"alias_kind":"pith_short_12","alias_value":"YSRT3Z23RYUZ","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YSRT3Z23RYUZTWCE","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YSRT3Z23","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:0dd99bace5d68b2a65af43b569d8f3a3456cfe37152586a9bc215cc1d17f2b63","target":"graph","created_at":"2026-05-18T00:40:56Z","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":"We consider acoustic wave transmission in non axisymmetric waveguide which consists of cylindrical resonator and two semi-infinite cylindrical waveguides whose axes are shifted relative to the resonator axis and each other by azimuthal angle $\\Delta\\phi$. We show that for rotation of one of attached waveguides the coupling matrix elements of the eigenmodes of resonator classified by the integer $m$ and propagating mode of the waveguide acquire phase factor $e^{im\\Delta\\phi}$. That crucially effect Fano resonances and creates an analog of faucet opening and closing wave flux under rotation of t","authors_text":"Alina A. Lyapina, Almas F. Sadreev, Artem S. Pilipchuk","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-04T09:06:37Z","title":"Tuning of bound states in the continuum by waveguide rotation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.00864","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":"sha256:4a0b6f41de75ed8c8f08fc06a4eb432ecc373976aae967a7ae750b97c45504cd","target":"record","created_at":"2026-05-18T00:40:56Z","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":"5af49d02242e95c5e93865a2564ca953b06398ac5db8dc58246d99f75d2a4d33","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-07-04T09:06:37Z","title_canon_sha256":"bdd5f9650061af896d2ef872a628aba40788d84d26ab6f24a36338ac63b64325"},"schema_version":"1.0","source":{"id":"1707.00864","kind":"arxiv","version":1}},"canonical_sha256":"c4a33de75b8e2999d8440fea567a1d91bc1882228bdc4f9f6f4bfcbc871a6c60","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c4a33de75b8e2999d8440fea567a1d91bc1882228bdc4f9f6f4bfcbc871a6c60","first_computed_at":"2026-05-18T00:40:56.791028Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:56.791028Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7Sm/3jU8Z1m7xBeYVDb5OzoC4Pw7S++0XNheNQUq7Wt9vrsevodGb+jwFwaP0rIKUZDZOqI+Lia2dNpGhoARBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:56.791615Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.00864","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4a0b6f41de75ed8c8f08fc06a4eb432ecc373976aae967a7ae750b97c45504cd","sha256:0dd99bace5d68b2a65af43b569d8f3a3456cfe37152586a9bc215cc1d17f2b63"],"state_sha256":"0cd12457238283f62a18380921226c45bbdbc0bd057a4ca21daa1bdfdd5a25b7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6qupdRtbEzJoENu2ir7QihZlUuxadSg4dhrF2n6mmiugsAyZQAADkUnLZ7UipRzYgwq/SacJe5O3Xq9clDkoCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T18:33:23.197269Z","bundle_sha256":"19d9b650cff61f08997c77f29948949c910fe07795cebbbc7ad4460e5f5e86aa"}}