{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:VB3MUZRVTR3HU7AKCM5ULGIC6V","short_pith_number":"pith:VB3MUZRV","schema_version":"1.0","canonical_sha256":"a876ca66359c767a7c0a133b459902f54510470bc52472a8db254d28ea3ae697","source":{"kind":"arxiv","id":"2201.07455","version":2},"attestation_state":"computed","paper":{"title":"Slow Electronic Dynamics in the Paramagnetic State of UTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Ai Nakamura, Dai Aoki, DeXin Li, Fuminori Honda, Hiroki Fujibayashi, Hironori Sakai, Katsuki Kinjo, Kenji Ishida, Petr Opletal, Shinsaku Kambe, Shunsaku Kitagawa, Yoshifumi Tokiwa, Yoshinori Haga, Yoshiya Homma, Yo Tokunaga, Yusei Shimizu","submitted_at":"2022-01-19T07:47:08Z","abstract_excerpt":"$^{125}$Te NMR experiments in field ($H$) applied along the easy magnetization axis (the $a$-axis) revealed slow electronic dynamics developing in the paramagnetic state of UTe$_2$. The observed slow fluctuations are concerned with a successive growth of long-range electronic correlations below 30$-$40 K, where the spin susceptibility along the hard magnetization axis (the $b$-axis) shows a broad maximum. The experiments also imply that tiny amounts of disorder or defects locally disturb the long-range electronic correlations and develop an inhomogeneous electronic state at low temperatures, l"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2201.07455","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-01-19T07:47:08Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"fbf856a20ee01e45b601c7ee636e903e41f1f432a0a6298db6deaf8b773a4fe1","abstract_canon_sha256":"7881ca1ec2bfc462a754f19b975093098d11efc50da6782686ea7b0ab7d3c158"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:54:04.428206Z","signature_b64":"cCpXidzxBOTxGNSY2BDpvld5g3Gu8dlQ5Z2BaGtxRRwWQuNRevOpzXrlgZxUbFYxXsYzOiAcYoCXh7oRPiaTCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a876ca66359c767a7c0a133b459902f54510470bc52472a8db254d28ea3ae697","last_reissued_at":"2026-07-05T03:54:04.427832Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:54:04.427832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Slow Electronic Dynamics in the Paramagnetic State of UTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Ai Nakamura, Dai Aoki, DeXin Li, Fuminori Honda, Hiroki Fujibayashi, Hironori Sakai, Katsuki Kinjo, Kenji Ishida, Petr Opletal, Shinsaku Kambe, Shunsaku Kitagawa, Yoshifumi Tokiwa, Yoshinori Haga, Yoshiya Homma, Yo Tokunaga, Yusei Shimizu","submitted_at":"2022-01-19T07:47:08Z","abstract_excerpt":"$^{125}$Te NMR experiments in field ($H$) applied along the easy magnetization axis (the $a$-axis) revealed slow electronic dynamics developing in the paramagnetic state of UTe$_2$. The observed slow fluctuations are concerned with a successive growth of long-range electronic correlations below 30$-$40 K, where the spin susceptibility along the hard magnetization axis (the $b$-axis) shows a broad maximum. The experiments also imply that tiny amounts of disorder or defects locally disturb the long-range electronic correlations and develop an inhomogeneous electronic state at low temperatures, l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2201.07455","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2201.07455/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2201.07455","created_at":"2026-07-05T03:54:04.427890+00:00"},{"alias_kind":"arxiv_version","alias_value":"2201.07455v2","created_at":"2026-07-05T03:54:04.427890+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2201.07455","created_at":"2026-07-05T03:54:04.427890+00:00"},{"alias_kind":"pith_short_12","alias_value":"VB3MUZRVTR3H","created_at":"2026-07-05T03:54:04.427890+00:00"},{"alias_kind":"pith_short_16","alias_value":"VB3MUZRVTR3HU7AK","created_at":"2026-07-05T03:54:04.427890+00:00"},{"alias_kind":"pith_short_8","alias_value":"VB3MUZRV","created_at":"2026-07-05T03:54:04.427890+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V","json":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V.json","graph_json":"https://pith.science/api/pith-number/VB3MUZRVTR3HU7AKCM5ULGIC6V/graph.json","events_json":"https://pith.science/api/pith-number/VB3MUZRVTR3HU7AKCM5ULGIC6V/events.json","paper":"https://pith.science/paper/VB3MUZRV"},"agent_actions":{"view_html":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V","download_json":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V.json","view_paper":"https://pith.science/paper/VB3MUZRV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2201.07455&json=true","fetch_graph":"https://pith.science/api/pith-number/VB3MUZRVTR3HU7AKCM5ULGIC6V/graph.json","fetch_events":"https://pith.science/api/pith-number/VB3MUZRVTR3HU7AKCM5ULGIC6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V/action/storage_attestation","attest_author":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V/action/author_attestation","sign_citation":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V/action/citation_signature","submit_replication":"https://pith.science/pith/VB3MUZRVTR3HU7AKCM5ULGIC6V/action/replication_record"}},"created_at":"2026-07-05T03:54:04.427890+00:00","updated_at":"2026-07-05T03:54:04.427890+00:00"}