{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ETG5JMHXIC4ONQFR6QNC7SYLIJ","short_pith_number":"pith:ETG5JMHX","schema_version":"1.0","canonical_sha256":"24cdd4b0f740b8e6c0b1f41a2fcb0b4262e6d6245506296e6c5e746d3bccf448","source":{"kind":"arxiv","id":"1712.10038","version":1},"attestation_state":"computed","paper":{"title":"Phononic thermal conductivity in silicene: the role of vacancy defects and boundary scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. Barati, M. Farmanbar, T. Salavati-fard, T. Vazifehshenas","submitted_at":"2017-12-28T19:55:36Z","abstract_excerpt":"We calculate the thermal conductivity of free-standing silicene using the phonon Boltzmann transport equation within the relaxation time approximation. In this calculation, we investigate the effects of sample size and different scattering mechanisms such as phonon-phonon, phonon-boundary, phonon-isotope and phonon-vacancy defect. Moreover, the role of different phonon modes is examined. We show that, in contrast to graphene, the dominant contribution to the thermal conductivity of silicene originates from the in-plane acoustic branches, which is about 70\\% at room temperature and this contrib"},"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":"1712.10038","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-12-28T19:55:36Z","cross_cats_sorted":[],"title_canon_sha256":"1701b0c9ebec5bdd27ee6049dd463df04f4b199748482bbb91ced1b73e24421b","abstract_canon_sha256":"86ffd1ebc62a889d34d2c3b27cc420e9f68c6999f93f0b6c357f994c4207dbfa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:14.196676Z","signature_b64":"SdJ94bh4c4M8FWaLyPamhKkrUwpxLm4sdtf3hEujVlibZ+oymSRBRP0q2S536UrlG3zXJ361yrkcI/fBwC7bBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"24cdd4b0f740b8e6c0b1f41a2fcb0b4262e6d6245506296e6c5e746d3bccf448","last_reissued_at":"2026-05-18T00:18:14.196230Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:14.196230Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phononic thermal conductivity in silicene: the role of vacancy defects and boundary scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. Barati, M. Farmanbar, T. Salavati-fard, T. Vazifehshenas","submitted_at":"2017-12-28T19:55:36Z","abstract_excerpt":"We calculate the thermal conductivity of free-standing silicene using the phonon Boltzmann transport equation within the relaxation time approximation. In this calculation, we investigate the effects of sample size and different scattering mechanisms such as phonon-phonon, phonon-boundary, phonon-isotope and phonon-vacancy defect. Moreover, the role of different phonon modes is examined. We show that, in contrast to graphene, the dominant contribution to the thermal conductivity of silicene originates from the in-plane acoustic branches, which is about 70\\% at room temperature and this contrib"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.10038","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":"1712.10038","created_at":"2026-05-18T00:18:14.196300+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.10038v1","created_at":"2026-05-18T00:18:14.196300+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.10038","created_at":"2026-05-18T00:18:14.196300+00:00"},{"alias_kind":"pith_short_12","alias_value":"ETG5JMHXIC4O","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"ETG5JMHXIC4ONQFR","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"ETG5JMHX","created_at":"2026-05-18T12:31:12.930513+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/ETG5JMHXIC4ONQFR6QNC7SYLIJ","json":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ.json","graph_json":"https://pith.science/api/pith-number/ETG5JMHXIC4ONQFR6QNC7SYLIJ/graph.json","events_json":"https://pith.science/api/pith-number/ETG5JMHXIC4ONQFR6QNC7SYLIJ/events.json","paper":"https://pith.science/paper/ETG5JMHX"},"agent_actions":{"view_html":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ","download_json":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ.json","view_paper":"https://pith.science/paper/ETG5JMHX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.10038&json=true","fetch_graph":"https://pith.science/api/pith-number/ETG5JMHXIC4ONQFR6QNC7SYLIJ/graph.json","fetch_events":"https://pith.science/api/pith-number/ETG5JMHXIC4ONQFR6QNC7SYLIJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ/action/storage_attestation","attest_author":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ/action/author_attestation","sign_citation":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ/action/citation_signature","submit_replication":"https://pith.science/pith/ETG5JMHXIC4ONQFR6QNC7SYLIJ/action/replication_record"}},"created_at":"2026-05-18T00:18:14.196300+00:00","updated_at":"2026-05-18T00:18:14.196300+00:00"}