{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:S562ZYLBHGV2MB24FCI3K2EVPC","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":"afbcf066bba9068cc7f1ab24ec95ef37a066c52f473144b6be82bf3f20688801","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-08-22T22:32:36Z","title_canon_sha256":"77517b9a8834a0ac0738314a38f14ccc1652cbd8c8290b2b881b02c3861266e3"},"schema_version":"1.0","source":{"id":"1608.06331","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.06331","created_at":"2026-05-18T00:54:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.06331v1","created_at":"2026-05-18T00:54:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.06331","created_at":"2026-05-18T00:54:19Z"},{"alias_kind":"pith_short_12","alias_value":"S562ZYLBHGV2","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"S562ZYLBHGV2MB24","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"S562ZYLB","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:5920165a741e4539097a7adea7b4676013495dbfd2a0ab1d3498b0cd90593a9f","target":"graph","created_at":"2026-05-18T00:54:19Z","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":"Anisotropy of the quadratic Zeeman effect for the $^3{\\rm H}_6 \\rightarrow \\, ^3{\\rm H}_4$ transition at 793 nm wavelength in $^{169}$Tm$^{3+}$-doped Y$_3$Al$_5$O$_{12}$ is studied, revealing shifts ranging from near zero up to + 4.69 GHz/T$^2$ for ions in magnetically inequivalent sites. This large range of shifts is used to spectrally resolve different subsets of ions and study nuclear spin relaxation as a function of temperature, magnetic field strength, and orientation in a site-selective manner. A rapid decrease in spin lifetime is found at large magnetic fields, revealing the weak contri","authors_text":"Charles W. Thiel, Lucile Veissier, Paul E. Barclay, Rufus L. Cone, Thomas Lutz, Wolfgang Tittel","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-08-22T22:32:36Z","title":"Quadratic Zeeman effect and spin-lattice relaxation of Tm$^{3+}$:YAG at high magnetic fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.06331","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:bd9e1ed1d6d68c3019dbb87026134fdaf1230372cefa00d9ff76b465bdd73408","target":"record","created_at":"2026-05-18T00:54:19Z","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":"afbcf066bba9068cc7f1ab24ec95ef37a066c52f473144b6be82bf3f20688801","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-08-22T22:32:36Z","title_canon_sha256":"77517b9a8834a0ac0738314a38f14ccc1652cbd8c8290b2b881b02c3861266e3"},"schema_version":"1.0","source":{"id":"1608.06331","kind":"arxiv","version":1}},"canonical_sha256":"977dace16139aba6075c2891b5689578bd95427dbc12444e3dd871992497aca0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"977dace16139aba6075c2891b5689578bd95427dbc12444e3dd871992497aca0","first_computed_at":"2026-05-18T00:54:19.765556Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:54:19.765556Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ymy0BIjyf6kQpdtUOFbntqyX7T+lDi1BreCI+wMeGi5o1vTX6wcPQjiYLMjgFe4vcjIvPg9CePSBu6AoV3PDCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:54:19.765960Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.06331","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd9e1ed1d6d68c3019dbb87026134fdaf1230372cefa00d9ff76b465bdd73408","sha256:5920165a741e4539097a7adea7b4676013495dbfd2a0ab1d3498b0cd90593a9f"],"state_sha256":"2f18643a1e092d4f628b8577fe0f97927fb9ccbb14409e5ac8403c64c6b55e34"}