{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OBSGQLPFVMWHSDWQLULCH4J5PR","short_pith_number":"pith:OBSGQLPF","schema_version":"1.0","canonical_sha256":"7064682de5ab2c790ed05d1623f13d7c6d611e8e0fcf38b3807f7df46b156999","source":{"kind":"arxiv","id":"1607.02360","version":3},"attestation_state":"computed","paper":{"title":"Nuclear Magnetic Resonance Reveals Disordered Level-Crossing Physics in the Bose-Glass Regime of the Br-doped Ni(Cl$_{1-x}$Br$_x$)$_2$-4SC(NH$_2$)$_2$ Compound at a High Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Anna Orlova, Armando Paduan-Filho, Claude Berthier, Edwin Kermarrec, Hadrien Mayaffre, Maxime Dupont, Mladen Horvati\\'c, Nicolas Laflorencie, R\\'emi Blinder, Sylvain Capponi","submitted_at":"2016-07-08T13:27:12Z","abstract_excerpt":"By measuring the nuclear magnetic resonance (NMR) 1/T_1 relaxation rate in the Br (bond) doped DTN compound, Ni(Cl(1-x)Br_x)2-4SC(NH2)2 (DTNX), we show that the low-energy spin dynamics of its high magnetic field \"Bose-glass\" regime is dominated by a strong peak of spin fluctuations found at the nearly doping-independent position H* = 13.6 T. From its temperature and field dependence we conclude that this corresponds to a level crossing of the energy levels related to the doping-induced impurity states. Observation of the local NMR signal from the spin adjacent to the doped Br allowed us to fu"},"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":"1607.02360","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-07-08T13:27:12Z","cross_cats_sorted":[],"title_canon_sha256":"f08c29a2e2bb4f4530048bf2eae3d17d52909fd99242a00d516cdd804215ddfd","abstract_canon_sha256":"ffcf2d2aff1384f65a935bd3364b50df35be82f80a145a1b841b6c2da9754eae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:01.234161Z","signature_b64":"sh1H+nib5/UXqLjsHcmhP9RnBYZpaYXZoguKdmWu7mxH19n8YdADIdYelW6g7w7AB0F1Un+P5dGTvrKRmj4cBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7064682de5ab2c790ed05d1623f13d7c6d611e8e0fcf38b3807f7df46b156999","last_reissued_at":"2026-05-18T00:51:01.233543Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:01.233543Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nuclear Magnetic Resonance Reveals Disordered Level-Crossing Physics in the Bose-Glass Regime of the Br-doped Ni(Cl$_{1-x}$Br$_x$)$_2$-4SC(NH$_2$)$_2$ Compound at a High Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Anna Orlova, Armando Paduan-Filho, Claude Berthier, Edwin Kermarrec, Hadrien Mayaffre, Maxime Dupont, Mladen Horvati\\'c, Nicolas Laflorencie, R\\'emi Blinder, Sylvain Capponi","submitted_at":"2016-07-08T13:27:12Z","abstract_excerpt":"By measuring the nuclear magnetic resonance (NMR) 1/T_1 relaxation rate in the Br (bond) doped DTN compound, Ni(Cl(1-x)Br_x)2-4SC(NH2)2 (DTNX), we show that the low-energy spin dynamics of its high magnetic field \"Bose-glass\" regime is dominated by a strong peak of spin fluctuations found at the nearly doping-independent position H* = 13.6 T. From its temperature and field dependence we conclude that this corresponds to a level crossing of the energy levels related to the doping-induced impurity states. Observation of the local NMR signal from the spin adjacent to the doped Br allowed us to fu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.02360","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1607.02360","created_at":"2026-05-18T00:51:01.233632+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.02360v3","created_at":"2026-05-18T00:51:01.233632+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.02360","created_at":"2026-05-18T00:51:01.233632+00:00"},{"alias_kind":"pith_short_12","alias_value":"OBSGQLPFVMWH","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OBSGQLPFVMWHSDWQ","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OBSGQLPF","created_at":"2026-05-18T12:30:36.002864+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/OBSGQLPFVMWHSDWQLULCH4J5PR","json":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR.json","graph_json":"https://pith.science/api/pith-number/OBSGQLPFVMWHSDWQLULCH4J5PR/graph.json","events_json":"https://pith.science/api/pith-number/OBSGQLPFVMWHSDWQLULCH4J5PR/events.json","paper":"https://pith.science/paper/OBSGQLPF"},"agent_actions":{"view_html":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR","download_json":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR.json","view_paper":"https://pith.science/paper/OBSGQLPF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.02360&json=true","fetch_graph":"https://pith.science/api/pith-number/OBSGQLPFVMWHSDWQLULCH4J5PR/graph.json","fetch_events":"https://pith.science/api/pith-number/OBSGQLPFVMWHSDWQLULCH4J5PR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR/action/storage_attestation","attest_author":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR/action/author_attestation","sign_citation":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR/action/citation_signature","submit_replication":"https://pith.science/pith/OBSGQLPFVMWHSDWQLULCH4J5PR/action/replication_record"}},"created_at":"2026-05-18T00:51:01.233632+00:00","updated_at":"2026-05-18T00:51:01.233632+00:00"}