{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:XTY3NQLORNXGLS7Q3DTSTZ36K5","short_pith_number":"pith:XTY3NQLO","canonical_record":{"source":{"id":"1710.11193","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-10-30T18:58:52Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"22cefcdc197171dcda101dae725205ddf1dbac1916682d5b6297ece1d0350da6","abstract_canon_sha256":"6fefb206bfe4897e9b635eabeeb3aa958ee19a0b388127880bf367e8653587aa"},"schema_version":"1.0"},"canonical_sha256":"bcf1b6c16e8b6e65cbf0d8e729e77e575da5722ae8a6a651adf13eb9da0d4659","source":{"kind":"arxiv","id":"1710.11193","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.11193","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"arxiv_version","alias_value":"1710.11193v1","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.11193","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"pith_short_12","alias_value":"XTY3NQLORNXG","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XTY3NQLORNXGLS7Q","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XTY3NQLO","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:XTY3NQLORNXGLS7Q3DTSTZ36K5","target":"record","payload":{"canonical_record":{"source":{"id":"1710.11193","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-10-30T18:58:52Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"22cefcdc197171dcda101dae725205ddf1dbac1916682d5b6297ece1d0350da6","abstract_canon_sha256":"6fefb206bfe4897e9b635eabeeb3aa958ee19a0b388127880bf367e8653587aa"},"schema_version":"1.0"},"canonical_sha256":"bcf1b6c16e8b6e65cbf0d8e729e77e575da5722ae8a6a651adf13eb9da0d4659","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:10.113551Z","signature_b64":"DdmjTPOK/VmVNjmYbxqLRG0bE1Mz8OmYXGOQkxyEu4jEXexwmjtMjclaaNSDnlFdp+8m+U2k57qjRQ2uSmDdCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bcf1b6c16e8b6e65cbf0d8e729e77e575da5722ae8a6a651adf13eb9da0d4659","last_reissued_at":"2026-05-18T00:21:10.112973Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:10.112973Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.11193","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":"2026-05-18T00:21:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Bnhz/RzOZJvoNLKAM6nZ7B7lLvg/VHxVIKLgGDoJvTIusjR6yYK/pWCgRI7R+7yoEIrAGwmpJVxLbzYNXOhxDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T20:30:13.625413Z"},"content_sha256":"fa166e1f9a4bb7a2b1e150959780471a433f82a536bb0861d645dc0b58df7c4b","schema_version":"1.0","event_id":"sha256:fa166e1f9a4bb7a2b1e150959780471a433f82a536bb0861d645dc0b58df7c4b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:XTY3NQLORNXGLS7Q3DTSTZ36K5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rayleigh-Brillouin light scattering spectroscopy of nitrous oxide (N$_2$O)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"physics.flu-dyn","authors_text":"K. Liang, W. Marques Jr., W. Ubachs, W. van de Water, Y. Wang","submitted_at":"2017-10-30T18:58:52Z","abstract_excerpt":"High signal-to-noise and high-resolution light scattering spectra are measured for nitrous oxide (N$_2$O) gas at an incident wavelength of 403.00 nm, at 90$^\\circ$ scattering, at room temperature and at gas pressures in the range $0.5-4$ bar. The resulting Rayleigh-Brillouin light scattering spectra are compared to a number of models describing in an approximate manner the collisional dynamics and energy transfer in this gaseous medium of this polyatomic molecular species. The Tenti-S6 model, based on macroscopic gas transport coefficients, reproduces the scattering profiles in the entire pres"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.11193","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":"2026-05-18T00:21:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vnAskoXkmtVfUps8Gu5qiTMLDXIXEOG+a8No4QEwR/cvWdntruqmz7gWpBQzp66Wk28dx58WS2PvJlv15fRsBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T20:30:13.625769Z"},"content_sha256":"b7d55a4903356bc54b5c01b64fdf0113b69f93ecd1cfb853e1befa89b539e725","schema_version":"1.0","event_id":"sha256:b7d55a4903356bc54b5c01b64fdf0113b69f93ecd1cfb853e1befa89b539e725"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/bundle.json","state_url":"https://pith.science/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/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":"2026-06-01T20:30:13Z","links":{"resolver":"https://pith.science/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5","bundle":"https://pith.science/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/bundle.json","state":"https://pith.science/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XTY3NQLORNXGLS7Q3DTSTZ36K5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:XTY3NQLORNXGLS7Q3DTSTZ36K5","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":"6fefb206bfe4897e9b635eabeeb3aa958ee19a0b388127880bf367e8653587aa","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-10-30T18:58:52Z","title_canon_sha256":"22cefcdc197171dcda101dae725205ddf1dbac1916682d5b6297ece1d0350da6"},"schema_version":"1.0","source":{"id":"1710.11193","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.11193","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"arxiv_version","alias_value":"1710.11193v1","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.11193","created_at":"2026-05-18T00:21:10Z"},{"alias_kind":"pith_short_12","alias_value":"XTY3NQLORNXG","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XTY3NQLORNXGLS7Q","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XTY3NQLO","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:b7d55a4903356bc54b5c01b64fdf0113b69f93ecd1cfb853e1befa89b539e725","target":"graph","created_at":"2026-05-18T00:21:10Z","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":"High signal-to-noise and high-resolution light scattering spectra are measured for nitrous oxide (N$_2$O) gas at an incident wavelength of 403.00 nm, at 90$^\\circ$ scattering, at room temperature and at gas pressures in the range $0.5-4$ bar. The resulting Rayleigh-Brillouin light scattering spectra are compared to a number of models describing in an approximate manner the collisional dynamics and energy transfer in this gaseous medium of this polyatomic molecular species. The Tenti-S6 model, based on macroscopic gas transport coefficients, reproduces the scattering profiles in the entire pres","authors_text":"K. Liang, W. Marques Jr., W. Ubachs, W. van de Water, Y. Wang","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-10-30T18:58:52Z","title":"Rayleigh-Brillouin light scattering spectroscopy of nitrous oxide (N$_2$O)"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.11193","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:fa166e1f9a4bb7a2b1e150959780471a433f82a536bb0861d645dc0b58df7c4b","target":"record","created_at":"2026-05-18T00:21:10Z","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":"6fefb206bfe4897e9b635eabeeb3aa958ee19a0b388127880bf367e8653587aa","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-10-30T18:58:52Z","title_canon_sha256":"22cefcdc197171dcda101dae725205ddf1dbac1916682d5b6297ece1d0350da6"},"schema_version":"1.0","source":{"id":"1710.11193","kind":"arxiv","version":1}},"canonical_sha256":"bcf1b6c16e8b6e65cbf0d8e729e77e575da5722ae8a6a651adf13eb9da0d4659","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bcf1b6c16e8b6e65cbf0d8e729e77e575da5722ae8a6a651adf13eb9da0d4659","first_computed_at":"2026-05-18T00:21:10.112973Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:21:10.112973Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DdmjTPOK/VmVNjmYbxqLRG0bE1Mz8OmYXGOQkxyEu4jEXexwmjtMjclaaNSDnlFdp+8m+U2k57qjRQ2uSmDdCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:21:10.113551Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.11193","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fa166e1f9a4bb7a2b1e150959780471a433f82a536bb0861d645dc0b58df7c4b","sha256:b7d55a4903356bc54b5c01b64fdf0113b69f93ecd1cfb853e1befa89b539e725"],"state_sha256":"e988dda78e631b38fa0c3b7d193f7373fce3b8f50c04c81d452709ffe1b44dc6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uxzeO35/gFunyd3oEaLBwsdSbJnMM6S3+zEkkoJsTclkMjFid4dDb/CA9E5N3EuVfJCe5DUZI40/S/jvs8UIAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T20:30:13.627992Z","bundle_sha256":"d5f7680b1fd0f45696dd8c035480c3b056e6580cec0f25e6b07125a456979ccf"}}