{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:XCRL34W5Q3L2YVOZ5RCD6LEBBW","short_pith_number":"pith:XCRL34W5","schema_version":"1.0","canonical_sha256":"b8a2bdf2dd86d7ac55d9ec443f2c810dbdf506c1e70cb459987e9212db7b2179","source":{"kind":"arxiv","id":"1610.02695","version":1},"attestation_state":"computed","paper":{"title":"Atomically inspired $k \\cdot p$ approach and valley Zeeman effect in transition metal dichalcogenide monolayers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"D. V. Rybkovskiy, I. C. Gerber, M. V. Durnev","submitted_at":"2016-10-09T17:05:25Z","abstract_excerpt":"We developed a six-band $k \\cdot p$ model that describes the electronic states of monolayer transition metal dichalcogenides (TMDCs) in $K$-valleys. The set of parameters for the $k \\cdot p$ model is uniquely determined by decomposing tight-binding (TB) models in the vicinity of $K^\\pm$-points. First, we used TB models existing in literature to derive systematic parametrizations for different materials, including MoS$_2$, WS$_2$, MoSe$_2$ and WSe$_2$. Then, by using the derived six-band $k \\cdot p$ Hamiltonian we calculated effective masses, Landau levels, and the effective exciton $g$-factor "},"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":"1610.02695","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-10-09T17:05:25Z","cross_cats_sorted":[],"title_canon_sha256":"577cb2b6776904a735a5e984141fbbadefc8dbbb4b6fffe4d2124b2ece486cad","abstract_canon_sha256":"e4e4beb34d6983dbe6e2cbacc34f408d972d97b8f67c566ac2e75781f166639f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:39.514011Z","signature_b64":"3p5BgfD3OdycKJrT0oGoYG17t/NBugz7krdwMrcwwiTjY3IQrQpiDxy6qIV3X6seKIATWlqyUUH/zlGN6C5rCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b8a2bdf2dd86d7ac55d9ec443f2c810dbdf506c1e70cb459987e9212db7b2179","last_reissued_at":"2026-05-18T00:46:39.513225Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:39.513225Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Atomically inspired $k \\cdot p$ approach and valley Zeeman effect in transition metal dichalcogenide monolayers","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"D. V. Rybkovskiy, I. C. Gerber, M. V. Durnev","submitted_at":"2016-10-09T17:05:25Z","abstract_excerpt":"We developed a six-band $k \\cdot p$ model that describes the electronic states of monolayer transition metal dichalcogenides (TMDCs) in $K$-valleys. The set of parameters for the $k \\cdot p$ model is uniquely determined by decomposing tight-binding (TB) models in the vicinity of $K^\\pm$-points. First, we used TB models existing in literature to derive systematic parametrizations for different materials, including MoS$_2$, WS$_2$, MoSe$_2$ and WSe$_2$. Then, by using the derived six-band $k \\cdot p$ Hamiltonian we calculated effective masses, Landau levels, and the effective exciton $g$-factor "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.02695","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":"1610.02695","created_at":"2026-05-18T00:46:39.513371+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.02695v1","created_at":"2026-05-18T00:46:39.513371+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.02695","created_at":"2026-05-18T00:46:39.513371+00:00"},{"alias_kind":"pith_short_12","alias_value":"XCRL34W5Q3L2","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_16","alias_value":"XCRL34W5Q3L2YVOZ","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_8","alias_value":"XCRL34W5","created_at":"2026-05-18T12:30:51.357362+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/XCRL34W5Q3L2YVOZ5RCD6LEBBW","json":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW.json","graph_json":"https://pith.science/api/pith-number/XCRL34W5Q3L2YVOZ5RCD6LEBBW/graph.json","events_json":"https://pith.science/api/pith-number/XCRL34W5Q3L2YVOZ5RCD6LEBBW/events.json","paper":"https://pith.science/paper/XCRL34W5"},"agent_actions":{"view_html":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW","download_json":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW.json","view_paper":"https://pith.science/paper/XCRL34W5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.02695&json=true","fetch_graph":"https://pith.science/api/pith-number/XCRL34W5Q3L2YVOZ5RCD6LEBBW/graph.json","fetch_events":"https://pith.science/api/pith-number/XCRL34W5Q3L2YVOZ5RCD6LEBBW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW/action/storage_attestation","attest_author":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW/action/author_attestation","sign_citation":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW/action/citation_signature","submit_replication":"https://pith.science/pith/XCRL34W5Q3L2YVOZ5RCD6LEBBW/action/replication_record"}},"created_at":"2026-05-18T00:46:39.513371+00:00","updated_at":"2026-05-18T00:46:39.513371+00:00"}