{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:F43DHPGFBIC6UBHIN2CT5WZTNC","short_pith_number":"pith:F43DHPGF","schema_version":"1.0","canonical_sha256":"2f3633bcc50a05ea04e86e853edb33688aa045dada8e6729bb6bb567fe1c2608","source":{"kind":"arxiv","id":"1801.02724","version":2},"attestation_state":"computed","paper":{"title":"Low frequency spin dynamics in XY quantum spin ice Yb$_2$Pt$_2$O$_7$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Arsenault, A. M. Hallas, C. Mauws, C. R. Wiebe, C. Sarkis, G. M. Luke, K. A. Ross, M. Tachibana, S. K. Takahashi, T. Imai","submitted_at":"2018-01-08T23:40:54Z","abstract_excerpt":"The XY pyrochlore Yb$_2$Ti$_2$O$_7$, with pseudo spin 1/2 at the Yb$^{3+}$ site, has been celebrated as potential host for the quantum spin ice state. The substitution of non-magnetic Ti with Pt gives Yb$_2$Pt$_2$O$_7$, a system with remarkably similar magnetic properties. The large nuclear gyromagnetic ratio ($\\gamma_{n}/2 \\pi = 9.15$~MHz/T) of $^{195}$Pt makes Yb$_2$Pt$_2$O$_7$ an ideal material for NMR investigation of its unconventional magnetic properties. Based on the $^{195}$Pt nuclear spin-lattice relaxation rate $1/T_1$ and the magnetic specific heat $C_{p}$ measured in a broad range "},"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":"1801.02724","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-08T23:40:54Z","cross_cats_sorted":[],"title_canon_sha256":"6fdcfb4d35332c7cc9ade74290f68f931ccf048164f7a4ad7e1e370390efa655","abstract_canon_sha256":"42134af41c0aa6e7222dff11b5155cc2df647ba2f4ed343d6697a1b803d8cc43"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:23.745589Z","signature_b64":"KBVMB/fvkqFW8rC3Co1XWttUn+s2ks2keS4MiL6QHSmTzPUALPRnW+U+NjZJXqpuVf3P8MWZUr2qPEPznNHxCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f3633bcc50a05ea04e86e853edb33688aa045dada8e6729bb6bb567fe1c2608","last_reissued_at":"2026-05-18T00:04:23.744757Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:23.744757Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low frequency spin dynamics in XY quantum spin ice Yb$_2$Pt$_2$O$_7$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Arsenault, A. M. Hallas, C. Mauws, C. R. Wiebe, C. Sarkis, G. M. Luke, K. A. Ross, M. Tachibana, S. K. Takahashi, T. Imai","submitted_at":"2018-01-08T23:40:54Z","abstract_excerpt":"The XY pyrochlore Yb$_2$Ti$_2$O$_7$, with pseudo spin 1/2 at the Yb$^{3+}$ site, has been celebrated as potential host for the quantum spin ice state. The substitution of non-magnetic Ti with Pt gives Yb$_2$Pt$_2$O$_7$, a system with remarkably similar magnetic properties. The large nuclear gyromagnetic ratio ($\\gamma_{n}/2 \\pi = 9.15$~MHz/T) of $^{195}$Pt makes Yb$_2$Pt$_2$O$_7$ an ideal material for NMR investigation of its unconventional magnetic properties. Based on the $^{195}$Pt nuclear spin-lattice relaxation rate $1/T_1$ and the magnetic specific heat $C_{p}$ measured in a broad range "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.02724","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":""},"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":"1801.02724","created_at":"2026-05-18T00:04:23.744893+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.02724v2","created_at":"2026-05-18T00:04:23.744893+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.02724","created_at":"2026-05-18T00:04:23.744893+00:00"},{"alias_kind":"pith_short_12","alias_value":"F43DHPGFBIC6","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_16","alias_value":"F43DHPGFBIC6UBHI","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_8","alias_value":"F43DHPGF","created_at":"2026-05-18T12:32:22.470017+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/F43DHPGFBIC6UBHIN2CT5WZTNC","json":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC.json","graph_json":"https://pith.science/api/pith-number/F43DHPGFBIC6UBHIN2CT5WZTNC/graph.json","events_json":"https://pith.science/api/pith-number/F43DHPGFBIC6UBHIN2CT5WZTNC/events.json","paper":"https://pith.science/paper/F43DHPGF"},"agent_actions":{"view_html":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC","download_json":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC.json","view_paper":"https://pith.science/paper/F43DHPGF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.02724&json=true","fetch_graph":"https://pith.science/api/pith-number/F43DHPGFBIC6UBHIN2CT5WZTNC/graph.json","fetch_events":"https://pith.science/api/pith-number/F43DHPGFBIC6UBHIN2CT5WZTNC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC/action/storage_attestation","attest_author":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC/action/author_attestation","sign_citation":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC/action/citation_signature","submit_replication":"https://pith.science/pith/F43DHPGFBIC6UBHIN2CT5WZTNC/action/replication_record"}},"created_at":"2026-05-18T00:04:23.744893+00:00","updated_at":"2026-05-18T00:04:23.744893+00:00"}