{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ZCB2SHLXQYAKSIZRQJ4JBCIUSV","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"48120bc5323972df9b5f7a2a797c9d8cf4eef75d5b53bd83433b439d108e2a2c","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-07-18T20:08:48Z","title_canon_sha256":"30c70ddf422b9f7588f12cbd5b25c6d5c04100b94f36f20230b531c5ec5e215f"},"schema_version":"1.0","source":{"id":"1807.07128","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.07128","created_at":"2026-05-18T00:00:51Z"},{"alias_kind":"arxiv_version","alias_value":"1807.07128v1","created_at":"2026-05-18T00:00:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.07128","created_at":"2026-05-18T00:00:51Z"},{"alias_kind":"pith_short_12","alias_value":"ZCB2SHLXQYAK","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_16","alias_value":"ZCB2SHLXQYAKSIZR","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_8","alias_value":"ZCB2SHLX","created_at":"2026-05-18T12:33:04Z"}],"graph_snapshots":[{"event_id":"sha256:b00a8a847d99f547ff65fe36795418dc0ca1e2fc4a78028b233d201e9d5f08b4","target":"graph","created_at":"2026-05-18T00:00:51Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"In-plane heterojunction tunnel field effect transistors based on monolayer transition metal dichalcogenides are studied by means of self-consistent non-equilibrium Green's functions simulations and an atomistic tight-binding Hamiltonian. We start by comparing several heterojunctions before focusing on the most promising ones, i.e WTe2-MoS2 and MoTe2-MoS2. The scalability of those devices as a function of channel length is studied, and the influence of backgate voltages on device performance is analysed. Our results indicate that, by fine-tuning the design parameters, those devices can yield ex","authors_text":"Efthimios Kaxiras, Jean Choukroun, Marco Pala, Philippe Dollfus, Shiang Fang","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-07-18T20:08:48Z","title":"High performance Tunnel Field Effect Transistors based on in-plane transition metal dichalcogenide heterojunctions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.07128","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:6a7943dfcd4cf059aef3604b1fac448bcfbd8d81bae48dad601f05a239e3603c","target":"record","created_at":"2026-05-18T00:00:51Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"48120bc5323972df9b5f7a2a797c9d8cf4eef75d5b53bd83433b439d108e2a2c","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2018-07-18T20:08:48Z","title_canon_sha256":"30c70ddf422b9f7588f12cbd5b25c6d5c04100b94f36f20230b531c5ec5e215f"},"schema_version":"1.0","source":{"id":"1807.07128","kind":"arxiv","version":1}},"canonical_sha256":"c883a91d778600a92331827890891495484929d2706c5e5ff5d9c4f32e3fc923","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c883a91d778600a92331827890891495484929d2706c5e5ff5d9c4f32e3fc923","first_computed_at":"2026-05-18T00:00:51.976712Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:51.976712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/3WIFrEmSKqwEjQ4dWoOjUj+cmDuXvUHDXWisfDhYZRw92i7ZqzAvkVa0XYzZB02kPAu+t6VXuQnzB0XxOSFCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:51.977279Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.07128","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6a7943dfcd4cf059aef3604b1fac448bcfbd8d81bae48dad601f05a239e3603c","sha256:b00a8a847d99f547ff65fe36795418dc0ca1e2fc4a78028b233d201e9d5f08b4"],"state_sha256":"dccefe00267d69eed10fb06e52640a1326f2ca24b5f9eebd6358fbcfaac6b63f"}