{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:VVJXM5QTP4ILLLWYSC7WLXMVGD","short_pith_number":"pith:VVJXM5QT","canonical_record":{"source":{"id":"1512.06306","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2015-12-20T02:27:33Z","cross_cats_sorted":["physics.optics","physics.plasm-ph"],"title_canon_sha256":"545bea894495adf927ad1949503284f222a74f2a45c1ee7699e7a7716b2ed7d2","abstract_canon_sha256":"3aaeceb41352ce26091a34bf09d74b1a594e6733aa5fe8e20f992b8ead59dd51"},"schema_version":"1.0"},"canonical_sha256":"ad537676137f10b5aed890bf65dd9530c368cff0276e195e9a7025dd820c271a","source":{"kind":"arxiv","id":"1512.06306","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.06306","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"arxiv_version","alias_value":"1512.06306v1","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.06306","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"pith_short_12","alias_value":"VVJXM5QTP4IL","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_16","alias_value":"VVJXM5QTP4ILLLWY","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_8","alias_value":"VVJXM5QT","created_at":"2026-05-18T12:29:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:VVJXM5QTP4ILLLWYSC7WLXMVGD","target":"record","payload":{"canonical_record":{"source":{"id":"1512.06306","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2015-12-20T02:27:33Z","cross_cats_sorted":["physics.optics","physics.plasm-ph"],"title_canon_sha256":"545bea894495adf927ad1949503284f222a74f2a45c1ee7699e7a7716b2ed7d2","abstract_canon_sha256":"3aaeceb41352ce26091a34bf09d74b1a594e6733aa5fe8e20f992b8ead59dd51"},"schema_version":"1.0"},"canonical_sha256":"ad537676137f10b5aed890bf65dd9530c368cff0276e195e9a7025dd820c271a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:00.891775Z","signature_b64":"c3KS3/YkygS+YMJwi655+qVg0lZXpx5l86D27FRTSzlWN1ArrDEiDozHNy6FKnw6bymnGqS2Rq4Z4QaiCx0ZCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad537676137f10b5aed890bf65dd9530c368cff0276e195e9a7025dd820c271a","last_reissued_at":"2026-05-18T01:24:00.891134Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:00.891134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.06306","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":"2026-05-18T01:24:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"W4m+9UP2awU+/siQgCWi540Jzb+MINgXUMbun/Xmi9A+b34ahcnJHAyn20p3DxDcTdzMEzBkn4xtjIyhVGcICQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T03:54:38.051741Z"},"content_sha256":"876e8ef216440db5123d25ddb84e4794163e2c5df27a3d93e9c42310bbe1243d","schema_version":"1.0","event_id":"sha256:876e8ef216440db5123d25ddb84e4794163e2c5df27a3d93e9c42310bbe1243d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:VVJXM5QTP4ILLLWYSC7WLXMVGD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tables of Einstein coefficients and lifetimes of upper rovibronic levels for Q-branch lines of the the $d^3\\Pi_u^- - a^3\\Sigma_g^+$ bands for the $H_2$, HD, $D_2$, and $T_2$ molecules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","physics.plasm-ph"],"primary_cat":"physics.chem-ph","authors_text":"B. P. Lavrov, L. L. Pozdeev, V. I. Yakovleva","submitted_at":"2015-12-20T02:27:33Z","abstract_excerpt":"The present work reports results of the semi-empirical determination of the spontaneous emission transition probabilities (Einstein coefficients) for Q-branch lines of Fulcher-$\\alpha$ band system and radiative lifetimes of upper electronic-vibro-rotational (rovibronic) levels for the most important isotopologues of diatomic hydrogen. They are based on an adiabatic theoretical model and all currently available experimental data on rovibronic energy levels, ratios of the line strengths and the lifetimes. Numerical data are presented in tabular format for vibrational quantum numbers v=0-7 (N is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.06306","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":"2026-05-18T01:24:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XbsTFJ8Hm25nomtaAXqjkLs7Naik4yz39Uc3HTcBTnqUumEtB6EIWxhr/iHhNikEuu7zfODFLEQo3XY9tcl2DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T03:54:38.052093Z"},"content_sha256":"113e196801f9e553c1c801cd31e713db45394c502b5533290629b661be64cf9f","schema_version":"1.0","event_id":"sha256:113e196801f9e553c1c801cd31e713db45394c502b5533290629b661be64cf9f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/bundle.json","state_url":"https://pith.science/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/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":"2026-06-25T03:54:38Z","links":{"resolver":"https://pith.science/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD","bundle":"https://pith.science/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/bundle.json","state":"https://pith.science/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VVJXM5QTP4ILLLWYSC7WLXMVGD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:VVJXM5QTP4ILLLWYSC7WLXMVGD","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":"3aaeceb41352ce26091a34bf09d74b1a594e6733aa5fe8e20f992b8ead59dd51","cross_cats_sorted":["physics.optics","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2015-12-20T02:27:33Z","title_canon_sha256":"545bea894495adf927ad1949503284f222a74f2a45c1ee7699e7a7716b2ed7d2"},"schema_version":"1.0","source":{"id":"1512.06306","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.06306","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"arxiv_version","alias_value":"1512.06306v1","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.06306","created_at":"2026-05-18T01:24:00Z"},{"alias_kind":"pith_short_12","alias_value":"VVJXM5QTP4IL","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_16","alias_value":"VVJXM5QTP4ILLLWY","created_at":"2026-05-18T12:29:47Z"},{"alias_kind":"pith_short_8","alias_value":"VVJXM5QT","created_at":"2026-05-18T12:29:47Z"}],"graph_snapshots":[{"event_id":"sha256:113e196801f9e553c1c801cd31e713db45394c502b5533290629b661be64cf9f","target":"graph","created_at":"2026-05-18T01:24:00Z","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 present work reports results of the semi-empirical determination of the spontaneous emission transition probabilities (Einstein coefficients) for Q-branch lines of Fulcher-$\\alpha$ band system and radiative lifetimes of upper electronic-vibro-rotational (rovibronic) levels for the most important isotopologues of diatomic hydrogen. They are based on an adiabatic theoretical model and all currently available experimental data on rovibronic energy levels, ratios of the line strengths and the lifetimes. Numerical data are presented in tabular format for vibrational quantum numbers v=0-7 (N is ","authors_text":"B. P. Lavrov, L. L. Pozdeev, V. I. Yakovleva","cross_cats":["physics.optics","physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2015-12-20T02:27:33Z","title":"Tables of Einstein coefficients and lifetimes of upper rovibronic levels for Q-branch lines of the the $d^3\\Pi_u^- - a^3\\Sigma_g^+$ bands for the $H_2$, HD, $D_2$, and $T_2$ molecules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.06306","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":"sha256:876e8ef216440db5123d25ddb84e4794163e2c5df27a3d93e9c42310bbe1243d","target":"record","created_at":"2026-05-18T01:24:00Z","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":"3aaeceb41352ce26091a34bf09d74b1a594e6733aa5fe8e20f992b8ead59dd51","cross_cats_sorted":["physics.optics","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2015-12-20T02:27:33Z","title_canon_sha256":"545bea894495adf927ad1949503284f222a74f2a45c1ee7699e7a7716b2ed7d2"},"schema_version":"1.0","source":{"id":"1512.06306","kind":"arxiv","version":1}},"canonical_sha256":"ad537676137f10b5aed890bf65dd9530c368cff0276e195e9a7025dd820c271a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ad537676137f10b5aed890bf65dd9530c368cff0276e195e9a7025dd820c271a","first_computed_at":"2026-05-18T01:24:00.891134Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:24:00.891134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"c3KS3/YkygS+YMJwi655+qVg0lZXpx5l86D27FRTSzlWN1ArrDEiDozHNy6FKnw6bymnGqS2Rq4Z4QaiCx0ZCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:24:00.891775Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.06306","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:876e8ef216440db5123d25ddb84e4794163e2c5df27a3d93e9c42310bbe1243d","sha256:113e196801f9e553c1c801cd31e713db45394c502b5533290629b661be64cf9f"],"state_sha256":"edef0e561260a8cc86f784bef728515f751b94a292aa1005430c11d6952429ca"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UYAjkDC/Sz23cDHJqqlwwyaaLUwEeoYItwUECoFjboMAGQvCLzEfZOQn6cMBJhjUV+wp5fgDnvOBCK5+ithtDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T03:54:38.054127Z","bundle_sha256":"cb65cee5f990655bd192f2a51bff37625a2c1cfda2d1de9c829586cebd6ab41c"}}