{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:DJRVP3NHSRFNINUNGSKLRJZFDV","short_pith_number":"pith:DJRVP3NH","schema_version":"1.0","canonical_sha256":"1a6357eda7944ad4368d3494b8a7251d7351fa3a531dc3f3c95804aabbbd7e8c","source":{"kind":"arxiv","id":"1705.11189","version":2},"attestation_state":"computed","paper":{"title":"Quasiparticle Interference of Surface States in Type-II Weyl Semimetal WTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alexey A. Soluyanov, Lunyong Zhang, Quansheng Wu, Sang-Wook Cheong, Weida Wu, Wenhan Zhang","submitted_at":"2017-05-31T17:40:58Z","abstract_excerpt":"Topological Weyl semimetal (TWS) is a metal, where low energy excitations behave like Weyl fermions of high-energy physics. It was recently shown that due to the lower symmetry of condensed matter systems, they can realize two distinct types of Weyl fermions. The type-I Weyl fermion in a metal is formed by a linear crossing of two bands at a point in the crystalline momentum space - Brillouin zone (BZ). The second type TWSs host type-II Weyl points appearing at the touching points of electron and hole pockets, which is a result of tilted linear dispersion. The type-II TWS was predicted to exis"},"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":"1705.11189","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-05-31T17:40:58Z","cross_cats_sorted":[],"title_canon_sha256":"af78e233a300ea5702a80175a93dc69a29154ff5bd77b9ebb2272ecf4292ace9","abstract_canon_sha256":"fbb264056d474affd974b3ba03876a67a580d9845ceb87658ccef7f6cc20772d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:42.984175Z","signature_b64":"n1RF0eSpoFL0kHorVSaECbUPOJ4ieN7p95gS1cmxllyZK7CINmyz9E3MBXa+KCJyRS1nj7KsAYUFnbdJLyvjDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a6357eda7944ad4368d3494b8a7251d7351fa3a531dc3f3c95804aabbbd7e8c","last_reissued_at":"2026-05-18T00:32:42.983486Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:42.983486Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quasiparticle Interference of Surface States in Type-II Weyl Semimetal WTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alexey A. Soluyanov, Lunyong Zhang, Quansheng Wu, Sang-Wook Cheong, Weida Wu, Wenhan Zhang","submitted_at":"2017-05-31T17:40:58Z","abstract_excerpt":"Topological Weyl semimetal (TWS) is a metal, where low energy excitations behave like Weyl fermions of high-energy physics. It was recently shown that due to the lower symmetry of condensed matter systems, they can realize two distinct types of Weyl fermions. The type-I Weyl fermion in a metal is formed by a linear crossing of two bands at a point in the crystalline momentum space - Brillouin zone (BZ). The second type TWSs host type-II Weyl points appearing at the touching points of electron and hole pockets, which is a result of tilted linear dispersion. The type-II TWS was predicted to exis"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.11189","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":"1705.11189","created_at":"2026-05-18T00:32:42.983589+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.11189v2","created_at":"2026-05-18T00:32:42.983589+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.11189","created_at":"2026-05-18T00:32:42.983589+00:00"},{"alias_kind":"pith_short_12","alias_value":"DJRVP3NHSRFN","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_16","alias_value":"DJRVP3NHSRFNINUN","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_8","alias_value":"DJRVP3NH","created_at":"2026-05-18T12:31:10.602751+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/DJRVP3NHSRFNINUNGSKLRJZFDV","json":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV.json","graph_json":"https://pith.science/api/pith-number/DJRVP3NHSRFNINUNGSKLRJZFDV/graph.json","events_json":"https://pith.science/api/pith-number/DJRVP3NHSRFNINUNGSKLRJZFDV/events.json","paper":"https://pith.science/paper/DJRVP3NH"},"agent_actions":{"view_html":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV","download_json":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV.json","view_paper":"https://pith.science/paper/DJRVP3NH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.11189&json=true","fetch_graph":"https://pith.science/api/pith-number/DJRVP3NHSRFNINUNGSKLRJZFDV/graph.json","fetch_events":"https://pith.science/api/pith-number/DJRVP3NHSRFNINUNGSKLRJZFDV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV/action/storage_attestation","attest_author":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV/action/author_attestation","sign_citation":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV/action/citation_signature","submit_replication":"https://pith.science/pith/DJRVP3NHSRFNINUNGSKLRJZFDV/action/replication_record"}},"created_at":"2026-05-18T00:32:42.983589+00:00","updated_at":"2026-05-18T00:32:42.983589+00:00"}