{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:UMBZBLB7ZB5LUKIFD3X4XSJYEC","short_pith_number":"pith:UMBZBLB7","canonical_record":{"source":{"id":"1704.00004","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-31T09:01:37Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"bf29207c73429672762203cd1bf904433731e66eadb2ec2685adb7a4f8235d54","abstract_canon_sha256":"1618dd3b0d8df19779e8385bdc6c55c1560aced0219ec1dc0a345d3c7ac997ef"},"schema_version":"1.0"},"canonical_sha256":"a30390ac3fc87aba29051eefcbc93820906c6afd19ab6413abae99f9989eefa0","source":{"kind":"arxiv","id":"1704.00004","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.00004","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"1704.00004v1","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.00004","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"UMBZBLB7ZB5L","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"UMBZBLB7ZB5LUKIF","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"UMBZBLB7","created_at":"2026-05-18T12:31:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:UMBZBLB7ZB5LUKIFD3X4XSJYEC","target":"record","payload":{"canonical_record":{"source":{"id":"1704.00004","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-31T09:01:37Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"bf29207c73429672762203cd1bf904433731e66eadb2ec2685adb7a4f8235d54","abstract_canon_sha256":"1618dd3b0d8df19779e8385bdc6c55c1560aced0219ec1dc0a345d3c7ac997ef"},"schema_version":"1.0"},"canonical_sha256":"a30390ac3fc87aba29051eefcbc93820906c6afd19ab6413abae99f9989eefa0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:56.034444Z","signature_b64":"2KjBAYNbtFJto7h+yPc43+nVPhoGoZHJrqaWX+GQWNs5jNvopGvYFsKAUUOnbHlMtgE0h3AxmxshOcRpju+BCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a30390ac3fc87aba29051eefcbc93820906c6afd19ab6413abae99f9989eefa0","last_reissued_at":"2026-05-18T00:38:56.033933Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:56.033933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.00004","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":"2026-05-18T00:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q7aBQJ1IxUIEgB4pYAAImGRFN8WM5fmGyL+I7Yrhyy5sbJbxijNDYOtKmTThcHCYXAGOHJz5bEIX/vPG0T2CAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T00:31:23.507625Z"},"content_sha256":"32f2a3ea0cc8b0b4b23a42cacd38e71cf53ff08e09c8d44312d2efc1cb5bf250","schema_version":"1.0","event_id":"sha256:32f2a3ea0cc8b0b4b23a42cacd38e71cf53ff08e09c8d44312d2efc1cb5bf250"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:UMBZBLB7ZB5LUKIFD3X4XSJYEC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Pulsed high magnetic field measurement via a Rubidium vapor sensor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"physics.atom-ph","authors_text":"Carlo Rizzo, Donatella Ciampini, Ennio Arimondo, J\\'er\\^ome B\\'eard, Nicolas Bruyant, Remy Battesti, Stefano Scotto, Sylvie George","submitted_at":"2017-03-31T09:01:37Z","abstract_excerpt":"We present a new technique to measure pulsed magnetic fields based on the use of Rubidium in gas phase as a metrological standard. We have therefore developed an instrument based on laser inducing transitions at about 780~nm (D2 line) in a Rubidium gas contained in a mini-cell of 3~mm~x~3~mm cross section. To be able to insert such a cell in a standard high field pulsed magnet we have realized a fibred probe kept at a fixed temperature. Transition frequencies for both the $\\pi$ (light polarization parallel to the magnetic field) and $\\sigma$ (light polarization perpendicular to the magnetic fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.00004","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":"2026-05-18T00:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t9W3HLuFPuKyITHzdmJo5jghCfSB4SMcsAAUQ0ifrSkfUL647w+dyPGtVyMb9HbP04sDT587pU6rKh6ZkpT0Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T00:31:23.507978Z"},"content_sha256":"03b73dcd1ecfe9ebe8a003a475ed84b29d94350e96ef11d1bd25e53dd749dccc","schema_version":"1.0","event_id":"sha256:03b73dcd1ecfe9ebe8a003a475ed84b29d94350e96ef11d1bd25e53dd749dccc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/bundle.json","state_url":"https://pith.science/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/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":"2026-05-31T00:31:23Z","links":{"resolver":"https://pith.science/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC","bundle":"https://pith.science/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/bundle.json","state":"https://pith.science/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UMBZBLB7ZB5LUKIFD3X4XSJYEC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:UMBZBLB7ZB5LUKIFD3X4XSJYEC","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":"1618dd3b0d8df19779e8385bdc6c55c1560aced0219ec1dc0a345d3c7ac997ef","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-31T09:01:37Z","title_canon_sha256":"bf29207c73429672762203cd1bf904433731e66eadb2ec2685adb7a4f8235d54"},"schema_version":"1.0","source":{"id":"1704.00004","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.00004","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"1704.00004v1","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.00004","created_at":"2026-05-18T00:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"UMBZBLB7ZB5L","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"UMBZBLB7ZB5LUKIF","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"UMBZBLB7","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:03b73dcd1ecfe9ebe8a003a475ed84b29d94350e96ef11d1bd25e53dd749dccc","target":"graph","created_at":"2026-05-18T00:38:56Z","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 present a new technique to measure pulsed magnetic fields based on the use of Rubidium in gas phase as a metrological standard. We have therefore developed an instrument based on laser inducing transitions at about 780~nm (D2 line) in a Rubidium gas contained in a mini-cell of 3~mm~x~3~mm cross section. To be able to insert such a cell in a standard high field pulsed magnet we have realized a fibred probe kept at a fixed temperature. Transition frequencies for both the $\\pi$ (light polarization parallel to the magnetic field) and $\\sigma$ (light polarization perpendicular to the magnetic fi","authors_text":"Carlo Rizzo, Donatella Ciampini, Ennio Arimondo, J\\'er\\^ome B\\'eard, Nicolas Bruyant, Remy Battesti, Stefano Scotto, Sylvie George","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-31T09:01:37Z","title":"Pulsed high magnetic field measurement via a Rubidium vapor sensor"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.00004","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":"sha256:32f2a3ea0cc8b0b4b23a42cacd38e71cf53ff08e09c8d44312d2efc1cb5bf250","target":"record","created_at":"2026-05-18T00:38:56Z","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":"1618dd3b0d8df19779e8385bdc6c55c1560aced0219ec1dc0a345d3c7ac997ef","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-03-31T09:01:37Z","title_canon_sha256":"bf29207c73429672762203cd1bf904433731e66eadb2ec2685adb7a4f8235d54"},"schema_version":"1.0","source":{"id":"1704.00004","kind":"arxiv","version":1}},"canonical_sha256":"a30390ac3fc87aba29051eefcbc93820906c6afd19ab6413abae99f9989eefa0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a30390ac3fc87aba29051eefcbc93820906c6afd19ab6413abae99f9989eefa0","first_computed_at":"2026-05-18T00:38:56.033933Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:56.033933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2KjBAYNbtFJto7h+yPc43+nVPhoGoZHJrqaWX+GQWNs5jNvopGvYFsKAUUOnbHlMtgE0h3AxmxshOcRpju+BCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:56.034444Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.00004","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:32f2a3ea0cc8b0b4b23a42cacd38e71cf53ff08e09c8d44312d2efc1cb5bf250","sha256:03b73dcd1ecfe9ebe8a003a475ed84b29d94350e96ef11d1bd25e53dd749dccc"],"state_sha256":"ab6dcaf93f0b488e9cdab1069caf763ceb52fba5e8c54ebf34aafa4c83062247"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8SyHbdTc5TqEmHC3fIZKjabxA3Q1Nsf6Hb/rBJZL9aABJ6ytec9EdK3yiQrGWZk1rfT27usGbBCW1eb88CE0Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T00:31:23.510332Z","bundle_sha256":"c3ea0f6dbacf371437d0c873f9eee8752e5b7d9348bffa6ab22f19e34c43bd15"}}