{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:AXNUXSAX3EB4QUEWRLVYAC32UU","short_pith_number":"pith:AXNUXSAX","schema_version":"1.0","canonical_sha256":"05db4bc817d903c850968aeb800b7aa52b6ffdf61f9f8a604cb6dce10647d170","source":{"kind":"arxiv","id":"1808.05981","version":3},"attestation_state":"computed","paper":{"title":"Emergence of topologically protected states in MoTe$_{2}$ Weyl semimetal with layer stacking order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chunruo Duan, Despina Louca, John A. Schneeloch, Junjie Yang, Jun Liu, Xiaoping Wang","submitted_at":"2018-08-17T20:19:45Z","abstract_excerpt":"Electronic tunability in crystals with weakly-bound layers can be achieved through layer stacking order. One such example is MoTe$_2$, where the low-temperature orthorhombic T$_d$ phase is topological and host to Weyl quasiparticles. The transition mechanism to the non-trivial topology is elucidated by single crystal neutron diffraction. Upon cooling from the monoclinic 1T$\\prime$ to the T$_d$ phase, diffuse scattering accompanies the transition, arising from random, in-plane layer displacements, and dissipates upon entering the T$_d$ phase. Diffuse scattering is observed only in the H0L plane"},"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":"1808.05981","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-08-17T20:19:45Z","cross_cats_sorted":[],"title_canon_sha256":"db0f19ad7cd38c64737bdd2632075886e802446241b1fb8ad47a51c831d98e21","abstract_canon_sha256":"e616fd53582f0a5e3e9f8021c9ad2f0bf16a0fb96c8d3f7fd2de085474a7ca6d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:33.901460Z","signature_b64":"CWpQwxpRUnL+sgQSJwlXYH4wJB3fil7s1fyZ/pLM3CHVWp+yAo6L+ksS9ezruGNjtMBIo/UtzPEnP1dwwndxAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"05db4bc817d903c850968aeb800b7aa52b6ffdf61f9f8a604cb6dce10647d170","last_reissued_at":"2026-05-17T23:48:33.900825Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:33.900825Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergence of topologically protected states in MoTe$_{2}$ Weyl semimetal with layer stacking order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chunruo Duan, Despina Louca, John A. Schneeloch, Junjie Yang, Jun Liu, Xiaoping Wang","submitted_at":"2018-08-17T20:19:45Z","abstract_excerpt":"Electronic tunability in crystals with weakly-bound layers can be achieved through layer stacking order. One such example is MoTe$_2$, where the low-temperature orthorhombic T$_d$ phase is topological and host to Weyl quasiparticles. The transition mechanism to the non-trivial topology is elucidated by single crystal neutron diffraction. Upon cooling from the monoclinic 1T$\\prime$ to the T$_d$ phase, diffuse scattering accompanies the transition, arising from random, in-plane layer displacements, and dissipates upon entering the T$_d$ phase. Diffuse scattering is observed only in the H0L plane"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.05981","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":"1808.05981","created_at":"2026-05-17T23:48:33.900920+00:00"},{"alias_kind":"arxiv_version","alias_value":"1808.05981v3","created_at":"2026-05-17T23:48:33.900920+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.05981","created_at":"2026-05-17T23:48:33.900920+00:00"},{"alias_kind":"pith_short_12","alias_value":"AXNUXSAX3EB4","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_16","alias_value":"AXNUXSAX3EB4QUEW","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_8","alias_value":"AXNUXSAX","created_at":"2026-05-18T12:32:13.499390+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/AXNUXSAX3EB4QUEWRLVYAC32UU","json":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU.json","graph_json":"https://pith.science/api/pith-number/AXNUXSAX3EB4QUEWRLVYAC32UU/graph.json","events_json":"https://pith.science/api/pith-number/AXNUXSAX3EB4QUEWRLVYAC32UU/events.json","paper":"https://pith.science/paper/AXNUXSAX"},"agent_actions":{"view_html":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU","download_json":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU.json","view_paper":"https://pith.science/paper/AXNUXSAX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1808.05981&json=true","fetch_graph":"https://pith.science/api/pith-number/AXNUXSAX3EB4QUEWRLVYAC32UU/graph.json","fetch_events":"https://pith.science/api/pith-number/AXNUXSAX3EB4QUEWRLVYAC32UU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU/action/storage_attestation","attest_author":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU/action/author_attestation","sign_citation":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU/action/citation_signature","submit_replication":"https://pith.science/pith/AXNUXSAX3EB4QUEWRLVYAC32UU/action/replication_record"}},"created_at":"2026-05-17T23:48:33.900920+00:00","updated_at":"2026-05-17T23:48:33.900920+00:00"}