{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:DYQTWM6OZAVJQIQAUHLLQE3M32","short_pith_number":"pith:DYQTWM6O","canonical_record":{"source":{"id":"1710.08589","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-10-24T03:32:10Z","cross_cats_sorted":[],"title_canon_sha256":"986916cb2a73128311fed40b794de67fe86e9935af79acb4b13eee7a623cd656","abstract_canon_sha256":"73e124fcb67ab4f7ff4e0afe07cf51d518ee7c300331b4dc7fa340b4634662ed"},"schema_version":"1.0"},"canonical_sha256":"1e213b33cec82a982200a1d6b8136cdeb71f38e469c403f7daf968400789b917","source":{"kind":"arxiv","id":"1710.08589","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.08589","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1710.08589v3","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.08589","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"DYQTWM6OZAVJ","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"DYQTWM6OZAVJQIQA","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"DYQTWM6O","created_at":"2026-05-18T12:31:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:DYQTWM6OZAVJQIQAUHLLQE3M32","target":"record","payload":{"canonical_record":{"source":{"id":"1710.08589","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-10-24T03:32:10Z","cross_cats_sorted":[],"title_canon_sha256":"986916cb2a73128311fed40b794de67fe86e9935af79acb4b13eee7a623cd656","abstract_canon_sha256":"73e124fcb67ab4f7ff4e0afe07cf51d518ee7c300331b4dc7fa340b4634662ed"},"schema_version":"1.0"},"canonical_sha256":"1e213b33cec82a982200a1d6b8136cdeb71f38e469c403f7daf968400789b917","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:10.141674Z","signature_b64":"NrtHzsRfdsKOlmSE/j3tIcb211QITZTfGnneMJ7GlrHmKitYpkH+l5efHiQxYm2Z+IrULu+Y7oKtG7vxBh5qCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e213b33cec82a982200a1d6b8136cdeb71f38e469c403f7daf968400789b917","last_reissued_at":"2026-05-17T23:59:10.141074Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:10.141074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.08589","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sbv6IzktgqfsGYChGJhMzWKo5/TMhgg1M4nDVsLHZREavEsDTFRNTT9dR0mwMP+coiJsnCbqAH5Hmu+9VLNnDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T09:57:37.776608Z"},"content_sha256":"efe094fa87207f2ab144df7345610f91e2b7c33ceda45344ab6e8f065bd71b42","schema_version":"1.0","event_id":"sha256:efe094fa87207f2ab144df7345610f91e2b7c33ceda45344ab6e8f065bd71b42"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:DYQTWM6OZAVJQIQAUHLLQE3M32","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Prospects for Polar Molecular Ion Optical Probe of Varying Proton-Electron Mass Ratio","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Brian C. Odom, Mark G. Kokish, Masatoshi Kajita, Patrick R. Stollenwerk","submitted_at":"2017-10-24T03:32:10Z","abstract_excerpt":"Molecules with deep vibrational potential wells provide optical intervals sensitive to variation in the proton-electron mass ratio ($\\mu$). On one hand, polar molecules are of interest since optical state preparation techniques have been demonstrated for such species. On the other hand, it might be assumed that polar species are unfavorable candidates, because typical molecule-frame dipole moments reduce vibrational state lifetimes and cause large polarizabilities and associated Stark shifts. Here, we consider single-photon spectroscopy on a vibrational overtone transition of the polar species"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.08589","kind":"arxiv","version":3},"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":"2026-05-17T23:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H9GRFSy6nnQhKw8/UwTqPDwT5QhSHbWRwnm/7eFr8jnmqA5eNnHHi4ZL1ot57o7I7AWNLalOioCty1M4sQp/DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T09:57:37.776951Z"},"content_sha256":"85634e0a655469d01499b3597966f1f53ab75a224335f0fd59f0e31b1191c72a","schema_version":"1.0","event_id":"sha256:85634e0a655469d01499b3597966f1f53ab75a224335f0fd59f0e31b1191c72a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/bundle.json","state_url":"https://pith.science/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/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":"2026-06-25T09:57:37Z","links":{"resolver":"https://pith.science/pith/DYQTWM6OZAVJQIQAUHLLQE3M32","bundle":"https://pith.science/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/bundle.json","state":"https://pith.science/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DYQTWM6OZAVJQIQAUHLLQE3M32/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:DYQTWM6OZAVJQIQAUHLLQE3M32","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":"73e124fcb67ab4f7ff4e0afe07cf51d518ee7c300331b4dc7fa340b4634662ed","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-10-24T03:32:10Z","title_canon_sha256":"986916cb2a73128311fed40b794de67fe86e9935af79acb4b13eee7a623cd656"},"schema_version":"1.0","source":{"id":"1710.08589","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.08589","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1710.08589v3","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.08589","created_at":"2026-05-17T23:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"DYQTWM6OZAVJ","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"DYQTWM6OZAVJQIQA","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"DYQTWM6O","created_at":"2026-05-18T12:31:12Z"}],"graph_snapshots":[{"event_id":"sha256:85634e0a655469d01499b3597966f1f53ab75a224335f0fd59f0e31b1191c72a","target":"graph","created_at":"2026-05-17T23:59:10Z","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":"Molecules with deep vibrational potential wells provide optical intervals sensitive to variation in the proton-electron mass ratio ($\\mu$). On one hand, polar molecules are of interest since optical state preparation techniques have been demonstrated for such species. On the other hand, it might be assumed that polar species are unfavorable candidates, because typical molecule-frame dipole moments reduce vibrational state lifetimes and cause large polarizabilities and associated Stark shifts. Here, we consider single-photon spectroscopy on a vibrational overtone transition of the polar species","authors_text":"Brian C. Odom, Mark G. Kokish, Masatoshi Kajita, Patrick R. Stollenwerk","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-10-24T03:32:10Z","title":"Prospects for Polar Molecular Ion Optical Probe of Varying Proton-Electron Mass Ratio"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.08589","kind":"arxiv","version":3},"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:efe094fa87207f2ab144df7345610f91e2b7c33ceda45344ab6e8f065bd71b42","target":"record","created_at":"2026-05-17T23:59:10Z","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":"73e124fcb67ab4f7ff4e0afe07cf51d518ee7c300331b4dc7fa340b4634662ed","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-10-24T03:32:10Z","title_canon_sha256":"986916cb2a73128311fed40b794de67fe86e9935af79acb4b13eee7a623cd656"},"schema_version":"1.0","source":{"id":"1710.08589","kind":"arxiv","version":3}},"canonical_sha256":"1e213b33cec82a982200a1d6b8136cdeb71f38e469c403f7daf968400789b917","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1e213b33cec82a982200a1d6b8136cdeb71f38e469c403f7daf968400789b917","first_computed_at":"2026-05-17T23:59:10.141074Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:10.141074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NrtHzsRfdsKOlmSE/j3tIcb211QITZTfGnneMJ7GlrHmKitYpkH+l5efHiQxYm2Z+IrULu+Y7oKtG7vxBh5qCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:10.141674Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.08589","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:efe094fa87207f2ab144df7345610f91e2b7c33ceda45344ab6e8f065bd71b42","sha256:85634e0a655469d01499b3597966f1f53ab75a224335f0fd59f0e31b1191c72a"],"state_sha256":"6e11ef15aa5effd1d57cf4a906c17ee1c4b31aa7c2103bc21327949521858e01"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iQHAjedUJi2uoRAsMM/691GSP/43/xJhXBNbLgjX+ARgNfyTVG4ujiri0tOZyUu4T5yQOjjrqQEPFgZNy5/BDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T09:57:37.778921Z","bundle_sha256":"f7515049e0075bf33dc57e55c41aec01358f37bf3adacad23d0d6bd9fef038c0"}}