{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:DQFY3SSOEBKATQQU547VPKRYAU","short_pith_number":"pith:DQFY3SSO","canonical_record":{"source":{"id":"2604.11457","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T13:34:48Z","cross_cats_sorted":[],"title_canon_sha256":"d0f01ad65283322e9e0adc94d7c2bb5db30607fa39f7c37b97e7f950a11419db","abstract_canon_sha256":"d5d0acf9babf0c9ba41bcb90f53d0202b547bf55e54538cd96c3c0f10a8a2846"},"schema_version":"1.0"},"canonical_sha256":"1c0b8dca4e205409c214ef3f57aa3805131ab699d65007b898b07c51696f4712","source":{"kind":"arxiv","id":"2604.11457","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11457","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11457v1","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11457","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_12","alias_value":"DQFY3SSOEBKA","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_16","alias_value":"DQFY3SSOEBKATQQU","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_8","alias_value":"DQFY3SSO","created_at":"2026-05-20T00:04:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:DQFY3SSOEBKATQQU547VPKRYAU","target":"record","payload":{"canonical_record":{"source":{"id":"2604.11457","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T13:34:48Z","cross_cats_sorted":[],"title_canon_sha256":"d0f01ad65283322e9e0adc94d7c2bb5db30607fa39f7c37b97e7f950a11419db","abstract_canon_sha256":"d5d0acf9babf0c9ba41bcb90f53d0202b547bf55e54538cd96c3c0f10a8a2846"},"schema_version":"1.0"},"canonical_sha256":"1c0b8dca4e205409c214ef3f57aa3805131ab699d65007b898b07c51696f4712","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:04:31.292642Z","signature_b64":"gCIPe7R/9rT7t5qQ8ZT/pQj2mlRb80ImxRhWCjIwmIfey1a48A3OMpUVYWeWW+ZuFPU1NVtVizmlivQidebtAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c0b8dca4e205409c214ef3f57aa3805131ab699d65007b898b07c51696f4712","last_reissued_at":"2026-05-20T00:04:31.291672Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:04:31.291672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2604.11457","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":"2026-05-20T00:04:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H/Crn5lYDf+4bXUPVVndyaRRPkdmSmTvDSPlx/f+k/ZPqa4CoslEvAX7/QMB7asSw4eGVLHygH/C7jBpq3LFDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:43:53.774597Z"},"content_sha256":"3f9349d5ef061890dbc6d935b2adcdc6f1f81ec851d6ca69f73d0b385c2033e2","schema_version":"1.0","event_id":"sha256:3f9349d5ef061890dbc6d935b2adcdc6f1f81ec851d6ca69f73d0b385c2033e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:DQFY3SSOEBKATQQU547VPKRYAU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite Vertical Windows: Seeing Only Part of the Picture in Rotating Turbulence","license":"http://creativecommons.org/licenses/by/4.0/","headline":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements.","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Eran Sharon, Omri Shaltiel","submitted_at":"2026-04-13T13:34:48Z","abstract_excerpt":"We report high-resolution measurements of three-dimensional (3D) turbulence in a rapidly rotating fluid. By decomposing the velocity field into a vertically averaged component and a three-dimensional residual, we show that each dominates distinct frequency ranges: the quasi-2D component at low frequencies and the 3D component at higher ones. This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically, revealing that the co"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That varying the vertical scan range isolates the effect of finite measurement windows without introducing confounding changes in the underlying turbulence, such as altered boundary conditions or forcing at different heights.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"The frequency crossover between quasi-2D and 3D regimes in rotating turbulence shifts systematically with vertical measurement span, showing the partition is shaped by finite observation windows rather than being intrinsic to the flow.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"138e1b66036b506258cf42a8f51640e65d8477ef3e71da5ab375781f2013efcd"},"source":{"id":"2604.11457","kind":"arxiv","version":1},"verdict":{"id":"426cdc04-923d-4d20-9e65-a294ce0beac9","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-10T16:04:40.732577Z","strongest_claim":"This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically.","one_line_summary":"The frequency crossover between quasi-2D and 3D regimes in rotating turbulence shifts systematically with vertical measurement span, showing the partition is shaped by finite observation windows rather than being intrinsic to the flow.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That varying the vertical scan range isolates the effect of finite measurement windows without introducing confounding changes in the underlying turbulence, such as altered boundary conditions or forcing at different heights.","pith_extraction_headline":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2604.11457/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":33,"sample":[{"doi":"","year":2018,"title":"Cascades and transitions in turbulent flows.Physics Reports, 767:1–101, 2018","work_id":"f227327c-e2be-4fa3-b4ff-de21afdd7d79","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2016,"title":"Coherent structures and extreme events in rotating multiphase turbulent flows.Physical Review X, 6(4):041036, 2016","work_id":"ddb40f7a-4a07-475e-aa54-b653650e08ef","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2015,"title":"Structure and dynamics of rotating turbulence: a review of recent experimental and numerical results.Applied Mechanics Reviews, 67(3), 2015","work_id":"788f20b7-a150-4fda-b476-39f814e91365","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2013,"title":"Cambridge University Press, 2013","work_id":"6d77b5ed-8993-4bba-b2b8-0466fd7f6e6b","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2003,"title":"Weak inertial-wave turbulence theory.Physical Review E, 68(1):015301, 2003","work_id":"392f4410-5112-491c-a909-08790b10ad9d","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":33,"snapshot_sha256":"e4d5b15d5cbd07f7a93fe47da9751234bebe5bfaa9fc807915ee22ceb4b9e058","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":"426cdc04-923d-4d20-9e65-a294ce0beac9"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:04:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GNdC1+76JkzNiYnvYJuj1nUQdU6M+S9pGVvcgSRmrcQbnQTQvynrt/JS4lrRELLPUNpyVi3ArsGVBDkreNhvCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:43:53.775283Z"},"content_sha256":"56006293338e7d43f4b1cba6a2cd51d73adf5c8be67c4ca7e268aaa224ab008a","schema_version":"1.0","event_id":"sha256:56006293338e7d43f4b1cba6a2cd51d73adf5c8be67c4ca7e268aaa224ab008a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DQFY3SSOEBKATQQU547VPKRYAU/bundle.json","state_url":"https://pith.science/pith/DQFY3SSOEBKATQQU547VPKRYAU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DQFY3SSOEBKATQQU547VPKRYAU/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":"2026-06-02T14:43:53Z","links":{"resolver":"https://pith.science/pith/DQFY3SSOEBKATQQU547VPKRYAU","bundle":"https://pith.science/pith/DQFY3SSOEBKATQQU547VPKRYAU/bundle.json","state":"https://pith.science/pith/DQFY3SSOEBKATQQU547VPKRYAU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DQFY3SSOEBKATQQU547VPKRYAU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:DQFY3SSOEBKATQQU547VPKRYAU","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":"d5d0acf9babf0c9ba41bcb90f53d0202b547bf55e54538cd96c3c0f10a8a2846","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T13:34:48Z","title_canon_sha256":"d0f01ad65283322e9e0adc94d7c2bb5db30607fa39f7c37b97e7f950a11419db"},"schema_version":"1.0","source":{"id":"2604.11457","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11457","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11457v1","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11457","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_12","alias_value":"DQFY3SSOEBKA","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_16","alias_value":"DQFY3SSOEBKATQQU","created_at":"2026-05-20T00:04:31Z"},{"alias_kind":"pith_short_8","alias_value":"DQFY3SSO","created_at":"2026-05-20T00:04:31Z"}],"graph_snapshots":[{"event_id":"sha256:56006293338e7d43f4b1cba6a2cd51d73adf5c8be67c4ca7e268aaa224ab008a","target":"graph","created_at":"2026-05-20T00:04:31Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That varying the vertical scan range isolates the effect of finite measurement windows without introducing confounding changes in the underlying turbulence, such as altered boundary conditions or forcing at different heights."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"The frequency crossover between quasi-2D and 3D regimes in rotating turbulence shifts systematically with vertical measurement span, showing the partition is shaped by finite observation windows rather than being intrinsic to the flow."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements."}],"snapshot_sha256":"138e1b66036b506258cf42a8f51640e65d8477ef3e71da5ab375781f2013efcd"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2604.11457/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We report high-resolution measurements of three-dimensional (3D) turbulence in a rapidly rotating fluid. By decomposing the velocity field into a vertically averaged component and a three-dimensional residual, we show that each dominates distinct frequency ranges: the quasi-2D component at low frequencies and the 3D component at higher ones. This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically, revealing that the co","authors_text":"Eran Sharon, Omri Shaltiel","cross_cats":[],"headline":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T13:34:48Z","title":"Finite Vertical Windows: Seeing Only Part of the Picture in Rotating Turbulence"},"references":{"count":33,"internal_anchors":0,"resolved_work":33,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Cascades and transitions in turbulent flows.Physics Reports, 767:1–101, 2018","work_id":"f227327c-e2be-4fa3-b4ff-de21afdd7d79","year":2018},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Coherent structures and extreme events in rotating multiphase turbulent flows.Physical Review X, 6(4):041036, 2016","work_id":"ddb40f7a-4a07-475e-aa54-b653650e08ef","year":2016},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"Structure and dynamics of rotating turbulence: a review of recent experimental and numerical results.Applied Mechanics Reviews, 67(3), 2015","work_id":"788f20b7-a150-4fda-b476-39f814e91365","year":2015},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Cambridge University Press, 2013","work_id":"6d77b5ed-8993-4bba-b2b8-0466fd7f6e6b","year":2013},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Weak inertial-wave turbulence theory.Physical Review E, 68(1):015301, 2003","work_id":"392f4410-5112-491c-a909-08790b10ad9d","year":2003}],"snapshot_sha256":"e4d5b15d5cbd07f7a93fe47da9751234bebe5bfaa9fc807915ee22ceb4b9e058"},"source":{"id":"2604.11457","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-10T16:04:40.732577Z","id":"426cdc04-923d-4d20-9e65-a294ce0beac9","model_set":{"reader":"grok-4.3"},"one_line_summary":"The frequency crossover between quasi-2D and 3D regimes in rotating turbulence shifts systematically with vertical measurement span, showing the partition is shaped by finite observation windows rather than being intrinsic to the flow.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The separation between 2D and 3D turbulence in rotating fluids depends on the vertical span of measurements.","strongest_claim":"This separation is not intrinsic to the flow but strongly depends on the finite vertical span of the measurements. As the vertical scan range increases, the apparent crossover between 2D and 3D-dominated regimes shifts systematically.","weakest_assumption":"That varying the vertical scan range isolates the effect of finite measurement windows without introducing confounding changes in the underlying turbulence, such as altered boundary conditions or forcing at different heights."}},"verdict_id":"426cdc04-923d-4d20-9e65-a294ce0beac9"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:3f9349d5ef061890dbc6d935b2adcdc6f1f81ec851d6ca69f73d0b385c2033e2","target":"record","created_at":"2026-05-20T00:04:31Z","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":"d5d0acf9babf0c9ba41bcb90f53d0202b547bf55e54538cd96c3c0f10a8a2846","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-04-13T13:34:48Z","title_canon_sha256":"d0f01ad65283322e9e0adc94d7c2bb5db30607fa39f7c37b97e7f950a11419db"},"schema_version":"1.0","source":{"id":"2604.11457","kind":"arxiv","version":1}},"canonical_sha256":"1c0b8dca4e205409c214ef3f57aa3805131ab699d65007b898b07c51696f4712","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1c0b8dca4e205409c214ef3f57aa3805131ab699d65007b898b07c51696f4712","first_computed_at":"2026-05-20T00:04:31.291672Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:04:31.291672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gCIPe7R/9rT7t5qQ8ZT/pQj2mlRb80ImxRhWCjIwmIfey1a48A3OMpUVYWeWW+ZuFPU1NVtVizmlivQidebtAA==","signature_status":"signed_v1","signed_at":"2026-05-20T00:04:31.292642Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.11457","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3f9349d5ef061890dbc6d935b2adcdc6f1f81ec851d6ca69f73d0b385c2033e2","sha256:56006293338e7d43f4b1cba6a2cd51d73adf5c8be67c4ca7e268aaa224ab008a"],"state_sha256":"e3224b9b766cb2a4d82d6817195ad36c107897becfdd4d605853e2cd9f4282cd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v8qr/jfBfqfj0NoU9BB1d6OWBs2TfWgZk3jOPh99CJBzkn3AnvAfSdrQFMNk5hbH1DyMYKI8527JPule/mNiAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T14:43:53.778007Z","bundle_sha256":"835001ef392f21d7ba156af22352045359b8743aa830125622bdd07f3ab0fd2e"}}