{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ATNBYUCUAXUJDTPE2SZOKSTSBJ","short_pith_number":"pith:ATNBYUCU","schema_version":"1.0","canonical_sha256":"04da1c505405e891cde4d4b2e54a720a656419354b9e4b1943c1da0db698903a","source":{"kind":"arxiv","id":"1706.03356","version":1},"attestation_state":"computed","paper":{"title":"The extremely large magnetoresistance in the Candidate Type-II Weyl semimetal MoTe2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"F. C. Chen, G. T. Lin, H. Y. Lv, Q. L. Pei, W. H. Song, W. J. Lu, X. B. Zhu, X. Luo, Y. P. Sun, Y. Y. Han","submitted_at":"2017-06-11T14:24:29Z","abstract_excerpt":"We performed the angle dependent magnetoresistance (MR), Hall effect measurements, the temperature dependent magneto-thermoelectric power (TEP) S(T) measurements, and the first-principles calculations to study the electronic properties of orthorhombic phase MoTe2 (Td-MoTe2), which was proposed to be electronically two-dimensional (2D). There are some interesting findings about Td-MoTe2: (1) A scaling approach {\\epsilon}{\\theta}=(sin2{\\theta}+{\\gamma}-2cos2{\\theta})1/2 is applied, where {\\theta} is the magnetic field angle with respect to the c axis of the crystal and {\\gamma} is the mass aniso"},"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":"1706.03356","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-11T14:24:29Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"e20e8f084936f1ba8ccf38266e8ed95ba9331dd75f8dd83da0368f4ab0b43b61","abstract_canon_sha256":"c277768a28d7033c59814f4698888fffb94cb3640d959c58fb0767d142e38e47"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:58.769529Z","signature_b64":"jg9WIWR65iORcbt8xMq6zfwrpWwrmESi39j7yD1JyYgkbxFDJLz+v+86tX7FtYqjijxgaH+4Ha6OeaVlKl86Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04da1c505405e891cde4d4b2e54a720a656419354b9e4b1943c1da0db698903a","last_reissued_at":"2026-05-18T00:41:58.768846Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:58.768846Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The extremely large magnetoresistance in the Candidate Type-II Weyl semimetal MoTe2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"F. C. Chen, G. T. Lin, H. Y. Lv, Q. L. Pei, W. H. Song, W. J. Lu, X. B. Zhu, X. Luo, Y. P. Sun, Y. Y. Han","submitted_at":"2017-06-11T14:24:29Z","abstract_excerpt":"We performed the angle dependent magnetoresistance (MR), Hall effect measurements, the temperature dependent magneto-thermoelectric power (TEP) S(T) measurements, and the first-principles calculations to study the electronic properties of orthorhombic phase MoTe2 (Td-MoTe2), which was proposed to be electronically two-dimensional (2D). There are some interesting findings about Td-MoTe2: (1) A scaling approach {\\epsilon}{\\theta}=(sin2{\\theta}+{\\gamma}-2cos2{\\theta})1/2 is applied, where {\\theta} is the magnetic field angle with respect to the c axis of the crystal and {\\gamma} is the mass aniso"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.03356","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":"1706.03356","created_at":"2026-05-18T00:41:58.768937+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.03356v1","created_at":"2026-05-18T00:41:58.768937+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.03356","created_at":"2026-05-18T00:41:58.768937+00:00"},{"alias_kind":"pith_short_12","alias_value":"ATNBYUCUAXUJ","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"ATNBYUCUAXUJDTPE","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"ATNBYUCU","created_at":"2026-05-18T12:31:08.081275+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/ATNBYUCUAXUJDTPE2SZOKSTSBJ","json":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ.json","graph_json":"https://pith.science/api/pith-number/ATNBYUCUAXUJDTPE2SZOKSTSBJ/graph.json","events_json":"https://pith.science/api/pith-number/ATNBYUCUAXUJDTPE2SZOKSTSBJ/events.json","paper":"https://pith.science/paper/ATNBYUCU"},"agent_actions":{"view_html":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ","download_json":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ.json","view_paper":"https://pith.science/paper/ATNBYUCU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.03356&json=true","fetch_graph":"https://pith.science/api/pith-number/ATNBYUCUAXUJDTPE2SZOKSTSBJ/graph.json","fetch_events":"https://pith.science/api/pith-number/ATNBYUCUAXUJDTPE2SZOKSTSBJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ/action/storage_attestation","attest_author":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ/action/author_attestation","sign_citation":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ/action/citation_signature","submit_replication":"https://pith.science/pith/ATNBYUCUAXUJDTPE2SZOKSTSBJ/action/replication_record"}},"created_at":"2026-05-18T00:41:58.768937+00:00","updated_at":"2026-05-18T00:41:58.768937+00:00"}