{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:WJKQLSSTTVF6WZRJWVT222P3CN","short_pith_number":"pith:WJKQLSST","schema_version":"1.0","canonical_sha256":"b25505ca539d4beb6629b567ad69fb1354f2e6cfc36b664f33ae53354ab600f7","source":{"kind":"arxiv","id":"1710.09571","version":1},"attestation_state":"computed","paper":{"title":"121,123Sb NQR as a microscopic probe in Te doped correlated semimetal FeSb2 : emergence of electronic Griffith phase, magnetism and metallic behavior %","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.A. Gippius, C. Petrovic, M. Baenitz, R. Hu, S. V. Zhurenko","submitted_at":"2017-10-26T07:49:09Z","abstract_excerpt":"$^{121,123}Sb$ nuclear quadrupole resonance (NQR) was applied to $Fe(Sb_{1-x}Te_x)_2$ in the low doping regime (\\emph{x = 0, 0.01} and \\emph{0.05}) as a microscopic zero field probe to study the evolution of \\emph{3d} magnetism and the emergence of metallic behavior. Whereas the NQR spectra itself reflects the degree of local disorder via the width of the individual NQR lines, the spin lattice relaxation rate (SLRR) $1/T_1(T)$ probes the fluctuations at the $Sb$ - site. The fluctuations originate either from conduction electrons or from magnetic moments. In contrast to the semi metal $FeSb_2$ "},"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":"1710.09571","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-10-26T07:49:09Z","cross_cats_sorted":[],"title_canon_sha256":"4bdadc7812e9e20be8545c0d554eb1c92fcefccbf152ce9c6abc86ae92f57399","abstract_canon_sha256":"e1205b2df334cbd2357fc34546a8b22ba871e246af456677a2e9a879b669d8e4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:58.138860Z","signature_b64":"EWeI/jkgFtkYANvlGsugHL+yHbkxbSlokzx9LsG+M0Sv5x7xU/6Fa88TgZDKhAa+S4AoA8aWcwNUl/EOfRc3AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b25505ca539d4beb6629b567ad69fb1354f2e6cfc36b664f33ae53354ab600f7","last_reissued_at":"2026-05-18T00:22:58.138219Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:58.138219Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"121,123Sb NQR as a microscopic probe in Te doped correlated semimetal FeSb2 : emergence of electronic Griffith phase, magnetism and metallic behavior %","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.A. Gippius, C. Petrovic, M. Baenitz, R. Hu, S. V. Zhurenko","submitted_at":"2017-10-26T07:49:09Z","abstract_excerpt":"$^{121,123}Sb$ nuclear quadrupole resonance (NQR) was applied to $Fe(Sb_{1-x}Te_x)_2$ in the low doping regime (\\emph{x = 0, 0.01} and \\emph{0.05}) as a microscopic zero field probe to study the evolution of \\emph{3d} magnetism and the emergence of metallic behavior. Whereas the NQR spectra itself reflects the degree of local disorder via the width of the individual NQR lines, the spin lattice relaxation rate (SLRR) $1/T_1(T)$ probes the fluctuations at the $Sb$ - site. The fluctuations originate either from conduction electrons or from magnetic moments. In contrast to the semi metal $FeSb_2$ "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.09571","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1710.09571","created_at":"2026-05-18T00:22:58.138326+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.09571v1","created_at":"2026-05-18T00:22:58.138326+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.09571","created_at":"2026-05-18T00:22:58.138326+00:00"},{"alias_kind":"pith_short_12","alias_value":"WJKQLSSTTVF6","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"WJKQLSSTTVF6WZRJ","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"WJKQLSST","created_at":"2026-05-18T12:31:53.515858+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/WJKQLSSTTVF6WZRJWVT222P3CN","json":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN.json","graph_json":"https://pith.science/api/pith-number/WJKQLSSTTVF6WZRJWVT222P3CN/graph.json","events_json":"https://pith.science/api/pith-number/WJKQLSSTTVF6WZRJWVT222P3CN/events.json","paper":"https://pith.science/paper/WJKQLSST"},"agent_actions":{"view_html":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN","download_json":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN.json","view_paper":"https://pith.science/paper/WJKQLSST","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.09571&json=true","fetch_graph":"https://pith.science/api/pith-number/WJKQLSSTTVF6WZRJWVT222P3CN/graph.json","fetch_events":"https://pith.science/api/pith-number/WJKQLSSTTVF6WZRJWVT222P3CN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN/action/storage_attestation","attest_author":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN/action/author_attestation","sign_citation":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN/action/citation_signature","submit_replication":"https://pith.science/pith/WJKQLSSTTVF6WZRJWVT222P3CN/action/replication_record"}},"created_at":"2026-05-18T00:22:58.138326+00:00","updated_at":"2026-05-18T00:22:58.138326+00:00"}