{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:76YCCFBELQ33WLOSPIVHGJITMN","short_pith_number":"pith:76YCCFBE","canonical_record":{"source":{"id":"1711.08033","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-11-21T20:47:49Z","cross_cats_sorted":[],"title_canon_sha256":"96940370f4138cc55654139fd533938c50bf598ee8d41842d5d0609297a0054d","abstract_canon_sha256":"60323767b5e86446e3a2a3d68930a3c96796c3cd2988f293435317aafc3d4b9e"},"schema_version":"1.0"},"canonical_sha256":"ffb02114245c37bb2dd27a2a732513637297227f84c95145d5da5fefb6b211ce","source":{"kind":"arxiv","id":"1711.08033","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.08033","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"1711.08033v1","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.08033","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"76YCCFBELQ33","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"76YCCFBELQ33WLOS","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"76YCCFBE","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:76YCCFBELQ33WLOSPIVHGJITMN","target":"record","payload":{"canonical_record":{"source":{"id":"1711.08033","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-11-21T20:47:49Z","cross_cats_sorted":[],"title_canon_sha256":"96940370f4138cc55654139fd533938c50bf598ee8d41842d5d0609297a0054d","abstract_canon_sha256":"60323767b5e86446e3a2a3d68930a3c96796c3cd2988f293435317aafc3d4b9e"},"schema_version":"1.0"},"canonical_sha256":"ffb02114245c37bb2dd27a2a732513637297227f84c95145d5da5fefb6b211ce","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:15.038711Z","signature_b64":"xigHjBcXDx5JXejrSoO62orvPok77pe9dYB28v7s8Wg4UvGHpqB5XAIFrz5WCDs8wqepwPoeQABgGRwQOwW0BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ffb02114245c37bb2dd27a2a732513637297227f84c95145d5da5fefb6b211ce","last_reissued_at":"2026-05-18T00:18:15.038286Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:15.038286Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.08033","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":"2026-05-18T00:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZbqYVHCmqtoirafSwZYZ3eB0MXFfiPUDzy1OEUXIXbNoGkfFaPrvqKKLv6bcf20NmbIGIKKA40zvMZAdKc/UAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:26:57.805334Z"},"content_sha256":"0bc84fef57016c9a8fe5fd29d65eb61e5019a4179a7f562faecd6acb98f79f5a","schema_version":"1.0","event_id":"sha256:0bc84fef57016c9a8fe5fd29d65eb61e5019a4179a7f562faecd6acb98f79f5a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:76YCCFBELQ33WLOSPIVHGJITMN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluorescence branching ratios and magnetic tuning of the visible spectrum of SrOH","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.chem-ph","authors_text":"Anne B. McCoy, Duc-Trung Nguyen, Ivan Kozyryev, Meng Huang, Timothy C. Steimle","submitted_at":"2017-11-21T20:47:49Z","abstract_excerpt":"The magnetic tuning of the low rotational levels in the Xsigma+(0,0,0), Api(0,0,0), and Bsigma+ (0,0,0) electronic states of strontium hydroxide, SrOH, have been experimentally investigated using high resolution optical Zeeman spectroscopy of a cold molecular beam sample. The observed Zeeman shifts and splittings are successfully modeled using a traditional effective Hamiltonian approach to account for the interaction between the Api and Bsigma+ states. The determined magnetic g-factors for the Xsigma+, Api , and Bsigma+ states are compared to those predicted by perturbation theory. The disper"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.08033","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":"2026-05-18T00:18:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pihuoroz+zGzSAfzxxgK09BfqTJPQCm5hbRP57imM9GNijhWsQW8ciMgI0eGq5+pAdEYONaCMVoQoMSeEydXDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:26:57.805978Z"},"content_sha256":"a46ad16bdcbc461a700b3bae8e0f7365ff0f2d5480a120e96d4e07f61aa3c35a","schema_version":"1.0","event_id":"sha256:a46ad16bdcbc461a700b3bae8e0f7365ff0f2d5480a120e96d4e07f61aa3c35a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/76YCCFBELQ33WLOSPIVHGJITMN/bundle.json","state_url":"https://pith.science/pith/76YCCFBELQ33WLOSPIVHGJITMN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/76YCCFBELQ33WLOSPIVHGJITMN/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":"2026-05-27T01:26:57Z","links":{"resolver":"https://pith.science/pith/76YCCFBELQ33WLOSPIVHGJITMN","bundle":"https://pith.science/pith/76YCCFBELQ33WLOSPIVHGJITMN/bundle.json","state":"https://pith.science/pith/76YCCFBELQ33WLOSPIVHGJITMN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/76YCCFBELQ33WLOSPIVHGJITMN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:76YCCFBELQ33WLOSPIVHGJITMN","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":"60323767b5e86446e3a2a3d68930a3c96796c3cd2988f293435317aafc3d4b9e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-11-21T20:47:49Z","title_canon_sha256":"96940370f4138cc55654139fd533938c50bf598ee8d41842d5d0609297a0054d"},"schema_version":"1.0","source":{"id":"1711.08033","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.08033","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"arxiv_version","alias_value":"1711.08033v1","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.08033","created_at":"2026-05-18T00:18:15Z"},{"alias_kind":"pith_short_12","alias_value":"76YCCFBELQ33","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"76YCCFBELQ33WLOS","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"76YCCFBE","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:a46ad16bdcbc461a700b3bae8e0f7365ff0f2d5480a120e96d4e07f61aa3c35a","target":"graph","created_at":"2026-05-18T00:18:15Z","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 magnetic tuning of the low rotational levels in the Xsigma+(0,0,0), Api(0,0,0), and Bsigma+ (0,0,0) electronic states of strontium hydroxide, SrOH, have been experimentally investigated using high resolution optical Zeeman spectroscopy of a cold molecular beam sample. The observed Zeeman shifts and splittings are successfully modeled using a traditional effective Hamiltonian approach to account for the interaction between the Api and Bsigma+ states. The determined magnetic g-factors for the Xsigma+, Api , and Bsigma+ states are compared to those predicted by perturbation theory. The disper","authors_text":"Anne B. McCoy, Duc-Trung Nguyen, Ivan Kozyryev, Meng Huang, Timothy C. Steimle","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-11-21T20:47:49Z","title":"Fluorescence branching ratios and magnetic tuning of the visible spectrum of SrOH"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.08033","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":"sha256:0bc84fef57016c9a8fe5fd29d65eb61e5019a4179a7f562faecd6acb98f79f5a","target":"record","created_at":"2026-05-18T00:18:15Z","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":"60323767b5e86446e3a2a3d68930a3c96796c3cd2988f293435317aafc3d4b9e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2017-11-21T20:47:49Z","title_canon_sha256":"96940370f4138cc55654139fd533938c50bf598ee8d41842d5d0609297a0054d"},"schema_version":"1.0","source":{"id":"1711.08033","kind":"arxiv","version":1}},"canonical_sha256":"ffb02114245c37bb2dd27a2a732513637297227f84c95145d5da5fefb6b211ce","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ffb02114245c37bb2dd27a2a732513637297227f84c95145d5da5fefb6b211ce","first_computed_at":"2026-05-18T00:18:15.038286Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:15.038286Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xigHjBcXDx5JXejrSoO62orvPok77pe9dYB28v7s8Wg4UvGHpqB5XAIFrz5WCDs8wqepwPoeQABgGRwQOwW0BA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:15.038711Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.08033","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0bc84fef57016c9a8fe5fd29d65eb61e5019a4179a7f562faecd6acb98f79f5a","sha256:a46ad16bdcbc461a700b3bae8e0f7365ff0f2d5480a120e96d4e07f61aa3c35a"],"state_sha256":"cc78b3b62f0273dbd9ca1c1609793eed83301be0e2f9ea0d936934f146b6a079"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yS8FEZPSXv526F9m+GBE8ynkcDjVYT1nLsEy+NZinVvj4VKZKfeOks9/PGwtidNTyJ3l+z0GH+iV5qOsC1QfCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T01:26:57.809697Z","bundle_sha256":"bab88f2b880c3cf33ec3c90d6e64f1e0e0b31a77b2df3c38c2d6d3afca5cb7f0"}}