{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:KISNRIIVMB4GVGN4XC7FBZXWL7","short_pith_number":"pith:KISNRIIV","schema_version":"1.0","canonical_sha256":"5224d8a11560786a99bcb8be50e6f65fe5ec5f4df0fa67bdc1e24269756c8f86","source":{"kind":"arxiv","id":"1806.03302","version":2},"attestation_state":"computed","paper":{"title":"Electronic properties of strained double-Weyl systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"E.V. Gorbar, I.A. Shovkovy, P.O. Sukhachov, V.A. Miransky","submitted_at":"2018-06-08T18:00:01Z","abstract_excerpt":"The effects of strains on the low-energy electronic properties of double-Weyl phases are studied in solids and cold-atom optical lattices. The principal finding is that deformations do not couple, in general, to the low-energy effective Hamiltonian as a pseudoelectromagnetic gauge potential. The response of an optical lattice to strains is simpler, but still only one of several strain-induced terms in the corresponding low-energy Hamiltonian can be interpreted as a gauge potential. Most interestingly, the strains can induce a nematic order parameter that splits a double-Weyl node into a pair o"},"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":"1806.03302","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-06-08T18:00:01Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a9a509ce54676551e461785b11963667dce59be6a244eed61be71a8cb1d1d615","abstract_canon_sha256":"16b267afaed3f97edf02ee7ebd1d74ca392e466158acd1cfce9a09b8b1648faf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:07:17.372651Z","signature_b64":"jJiYmxf/V0aUSptJfW0ZY3YXc2pJifSuzBSFVG/zy9+lfzverP6OuZkeef9Xfy9DlXHK3ONT+RbOmDzh80xWBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5224d8a11560786a99bcb8be50e6f65fe5ec5f4df0fa67bdc1e24269756c8f86","last_reissued_at":"2026-05-18T00:07:17.372080Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:07:17.372080Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electronic properties of strained double-Weyl systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"E.V. Gorbar, I.A. Shovkovy, P.O. Sukhachov, V.A. Miransky","submitted_at":"2018-06-08T18:00:01Z","abstract_excerpt":"The effects of strains on the low-energy electronic properties of double-Weyl phases are studied in solids and cold-atom optical lattices. The principal finding is that deformations do not couple, in general, to the low-energy effective Hamiltonian as a pseudoelectromagnetic gauge potential. The response of an optical lattice to strains is simpler, but still only one of several strain-induced terms in the corresponding low-energy Hamiltonian can be interpreted as a gauge potential. Most interestingly, the strains can induce a nematic order parameter that splits a double-Weyl node into a pair o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.03302","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":"1806.03302","created_at":"2026-05-18T00:07:17.372155+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.03302v2","created_at":"2026-05-18T00:07:17.372155+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.03302","created_at":"2026-05-18T00:07:17.372155+00:00"},{"alias_kind":"pith_short_12","alias_value":"KISNRIIVMB4G","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_16","alias_value":"KISNRIIVMB4GVGN4","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_8","alias_value":"KISNRIIV","created_at":"2026-05-18T12:32:33.847187+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/KISNRIIVMB4GVGN4XC7FBZXWL7","json":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7.json","graph_json":"https://pith.science/api/pith-number/KISNRIIVMB4GVGN4XC7FBZXWL7/graph.json","events_json":"https://pith.science/api/pith-number/KISNRIIVMB4GVGN4XC7FBZXWL7/events.json","paper":"https://pith.science/paper/KISNRIIV"},"agent_actions":{"view_html":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7","download_json":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7.json","view_paper":"https://pith.science/paper/KISNRIIV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.03302&json=true","fetch_graph":"https://pith.science/api/pith-number/KISNRIIVMB4GVGN4XC7FBZXWL7/graph.json","fetch_events":"https://pith.science/api/pith-number/KISNRIIVMB4GVGN4XC7FBZXWL7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7/action/storage_attestation","attest_author":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7/action/author_attestation","sign_citation":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7/action/citation_signature","submit_replication":"https://pith.science/pith/KISNRIIVMB4GVGN4XC7FBZXWL7/action/replication_record"}},"created_at":"2026-05-18T00:07:17.372155+00:00","updated_at":"2026-05-18T00:07:17.372155+00:00"}