{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:ASWM6YOJJURTOAPPXQVHPPBORE","short_pith_number":"pith:ASWM6YOJ","canonical_record":{"source":{"id":"1208.4939","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-08-24T09:51:47Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"83d0179bd3b0333d9f130f13003eabcccfdcc8f93edb66def120f1832cb4c2e4","abstract_canon_sha256":"98892c9d6bc978d31b0c3509c59860a8f94e98a4dc2dfe060a3a756f7b043cdf"},"schema_version":"1.0"},"canonical_sha256":"04accf61c94d233701efbc2a77bc2e892bd17e4058091e826a887e075e1bae19","source":{"kind":"arxiv","id":"1208.4939","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.4939","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"arxiv_version","alias_value":"1208.4939v1","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.4939","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"pith_short_12","alias_value":"ASWM6YOJJURT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"ASWM6YOJJURTOAPP","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"ASWM6YOJ","created_at":"2026-05-18T12:26:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:ASWM6YOJJURTOAPPXQVHPPBORE","target":"record","payload":{"canonical_record":{"source":{"id":"1208.4939","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-08-24T09:51:47Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"83d0179bd3b0333d9f130f13003eabcccfdcc8f93edb66def120f1832cb4c2e4","abstract_canon_sha256":"98892c9d6bc978d31b0c3509c59860a8f94e98a4dc2dfe060a3a756f7b043cdf"},"schema_version":"1.0"},"canonical_sha256":"04accf61c94d233701efbc2a77bc2e892bd17e4058091e826a887e075e1bae19","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:52.187759Z","signature_b64":"ut/DG05CiOjHVjZmZupULPo0eFzXYsEw3vL/QVo7Fzf3A46vTvOvyoxt5tAU5wJdWr99PoYqacj9GQ6D1SU2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04accf61c94d233701efbc2a77bc2e892bd17e4058091e826a887e075e1bae19","last_reissued_at":"2026-05-18T03:47:52.187347Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:52.187347Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1208.4939","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":"2026-05-18T03:47:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7uP5LnhkEOZkNkdGfsXEif30AKj/PvTGk1iZe/x6YkpbDWM2EwJqQ4FGcuJY79fnVy+AhlSf0F8r33OS6WR8CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T10:24:09.390947Z"},"content_sha256":"c1b0e989f61ac9f6b22c4a217d21fde37aa2e163f3cb5307b3ce394bf7d01086","schema_version":"1.0","event_id":"sha256:c1b0e989f61ac9f6b22c4a217d21fde37aa2e163f3cb5307b3ce394bf7d01086"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:ASWM6YOJJURTOAPPXQVHPPBORE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic dipole transitions in the OH $A\\,^2\\Sigma^+ \\leftarrow X\\,^2\\Pi$ system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.chem-ph","authors_text":"Ad van der Avoird, Gerard Meijer, Gerrit C. Groenenboom, Koos B. Gubbels, Moritz Kirste, Sebastiaan Y. T. van de Meerakker, Xingan Wang","submitted_at":"2012-08-24T09:51:47Z","abstract_excerpt":"We report on the observation of magnetic dipole allowed transitions in the well-characterized $A\\,^2\\Sigma^+ - X\\,^2\\Pi$ band system of the OH radical. A Stark decelerator in combination with microwave Rabi spectroscopy is used to control the populations in selected hyperfine levels of both $\\Lambda$-doublet components of the $X\\,^2\\Pi_{3/2},v=0,J=3/2$ ground state. Theoretical calculations presented in this paper predict that the magnetic dipole transitions in the $\\nu'=1 \\leftarrow \\nu=0$ band are weaker than the electric dipole transitions by a factor of $2.58\\times 10^3$ only, i.e., much l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.4939","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":"2026-05-18T03:47:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NG266m7FqxIUI1sIHQz+US7MqvInIL1oXl6JL6JpdEgS8KmrnxrgR3PaCV8Yiz1Zasx31gUFjMh15/NbRaMQDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T10:24:09.391288Z"},"content_sha256":"893b5209d3a785c9ba7b51b4f3f40e4ad71635b688795bd560b5b2d70ddc6496","schema_version":"1.0","event_id":"sha256:893b5209d3a785c9ba7b51b4f3f40e4ad71635b688795bd560b5b2d70ddc6496"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ASWM6YOJJURTOAPPXQVHPPBORE/bundle.json","state_url":"https://pith.science/pith/ASWM6YOJJURTOAPPXQVHPPBORE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ASWM6YOJJURTOAPPXQVHPPBORE/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":"2026-06-24T10:24:09Z","links":{"resolver":"https://pith.science/pith/ASWM6YOJJURTOAPPXQVHPPBORE","bundle":"https://pith.science/pith/ASWM6YOJJURTOAPPXQVHPPBORE/bundle.json","state":"https://pith.science/pith/ASWM6YOJJURTOAPPXQVHPPBORE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ASWM6YOJJURTOAPPXQVHPPBORE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:ASWM6YOJJURTOAPPXQVHPPBORE","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":"98892c9d6bc978d31b0c3509c59860a8f94e98a4dc2dfe060a3a756f7b043cdf","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-08-24T09:51:47Z","title_canon_sha256":"83d0179bd3b0333d9f130f13003eabcccfdcc8f93edb66def120f1832cb4c2e4"},"schema_version":"1.0","source":{"id":"1208.4939","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.4939","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"arxiv_version","alias_value":"1208.4939v1","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.4939","created_at":"2026-05-18T03:47:52Z"},{"alias_kind":"pith_short_12","alias_value":"ASWM6YOJJURT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"ASWM6YOJJURTOAPP","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"ASWM6YOJ","created_at":"2026-05-18T12:26:58Z"}],"graph_snapshots":[{"event_id":"sha256:893b5209d3a785c9ba7b51b4f3f40e4ad71635b688795bd560b5b2d70ddc6496","target":"graph","created_at":"2026-05-18T03:47:52Z","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 report on the observation of magnetic dipole allowed transitions in the well-characterized $A\\,^2\\Sigma^+ - X\\,^2\\Pi$ band system of the OH radical. A Stark decelerator in combination with microwave Rabi spectroscopy is used to control the populations in selected hyperfine levels of both $\\Lambda$-doublet components of the $X\\,^2\\Pi_{3/2},v=0,J=3/2$ ground state. Theoretical calculations presented in this paper predict that the magnetic dipole transitions in the $\\nu'=1 \\leftarrow \\nu=0$ band are weaker than the electric dipole transitions by a factor of $2.58\\times 10^3$ only, i.e., much l","authors_text":"Ad van der Avoird, Gerard Meijer, Gerrit C. Groenenboom, Koos B. Gubbels, Moritz Kirste, Sebastiaan Y. T. van de Meerakker, Xingan Wang","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-08-24T09:51:47Z","title":"Magnetic dipole transitions in the OH $A\\,^2\\Sigma^+ \\leftarrow X\\,^2\\Pi$ system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.4939","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:c1b0e989f61ac9f6b22c4a217d21fde37aa2e163f3cb5307b3ce394bf7d01086","target":"record","created_at":"2026-05-18T03:47:52Z","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":"98892c9d6bc978d31b0c3509c59860a8f94e98a4dc2dfe060a3a756f7b043cdf","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-08-24T09:51:47Z","title_canon_sha256":"83d0179bd3b0333d9f130f13003eabcccfdcc8f93edb66def120f1832cb4c2e4"},"schema_version":"1.0","source":{"id":"1208.4939","kind":"arxiv","version":1}},"canonical_sha256":"04accf61c94d233701efbc2a77bc2e892bd17e4058091e826a887e075e1bae19","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"04accf61c94d233701efbc2a77bc2e892bd17e4058091e826a887e075e1bae19","first_computed_at":"2026-05-18T03:47:52.187347Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:47:52.187347Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ut/DG05CiOjHVjZmZupULPo0eFzXYsEw3vL/QVo7Fzf3A46vTvOvyoxt5tAU5wJdWr99PoYqacj9GQ6D1SU2AA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:47:52.187759Z","signed_message":"canonical_sha256_bytes"},"source_id":"1208.4939","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c1b0e989f61ac9f6b22c4a217d21fde37aa2e163f3cb5307b3ce394bf7d01086","sha256:893b5209d3a785c9ba7b51b4f3f40e4ad71635b688795bd560b5b2d70ddc6496"],"state_sha256":"a7820b45c0b9e93ef52c0463c4409e261be2192edb03594b65754fe98e0801b1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7mSyOpA1dy82smOcIPqKIcDpatt4OkTrl3v2QPPUybyR8rGLEU51Eoq5YSc8z4bqo++atk8i2/w3lFsksLmdBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T10:24:09.393188Z","bundle_sha256":"9f1482c7d360fda99d4ebd8e0c3a3fad02771394d10706537af12b494f55f12e"}}