{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:YXIRUWD7CBBFQWXKGYC27CV2UX","short_pith_number":"pith:YXIRUWD7","schema_version":"1.0","canonical_sha256":"c5d11a587f1042585aea3605af8abaa5ca82216d3cb4a880918330e612ba07c2","source":{"kind":"arxiv","id":"0706.1012","version":1},"attestation_state":"computed","paper":{"title":"Ab initio melting curve of molybdenum by the phase coexistence method","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Cazorla, D. Alf\\`e, M. J. Gillan, S. Taioli","submitted_at":"2007-06-07T14:46:45Z","abstract_excerpt":"We report ab initio calculations of the melting curve of molybdenum for the pressure range 0-400 GPa. The calculations employ density functional theory (DFT) with the Perdew-Burke-Ernzerhof exchange-correlation functional in the projector augmented wave (PAW) implementation. We present tests showing that these techniques accurately reproduce experimental data on low-temperature b.c.c. Mo, and that PAW agrees closely with results from the full-potential linearized augmented plane-wave implementation. The work attempts to overcome the uncertainties inherent in earlier DFT calculations of the mel"},"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":"0706.1012","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2007-06-07T14:46:45Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"1d9910ad6d8b63c8541f8ddbbd5312a6d83bcc9167db3ea53793049586f20385","abstract_canon_sha256":"440eb4c860388177ae86692aa85a05c6b138a9841e83c29ba40a77c0891bb64e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:04:06.954146Z","signature_b64":"7lTDIxw9TPKWkD2r0RpLydZKlmAAgrAFbqgOK1zcxGykIXl5FXEn52JVdP9kuW9SNesW+lIW9IEtnBUy58MGAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5d11a587f1042585aea3605af8abaa5ca82216d3cb4a880918330e612ba07c2","last_reissued_at":"2026-07-04T17:04:06.953776Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:04:06.953776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ab initio melting curve of molybdenum by the phase coexistence method","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Cazorla, D. Alf\\`e, M. J. Gillan, S. Taioli","submitted_at":"2007-06-07T14:46:45Z","abstract_excerpt":"We report ab initio calculations of the melting curve of molybdenum for the pressure range 0-400 GPa. The calculations employ density functional theory (DFT) with the Perdew-Burke-Ernzerhof exchange-correlation functional in the projector augmented wave (PAW) implementation. We present tests showing that these techniques accurately reproduce experimental data on low-temperature b.c.c. Mo, and that PAW agrees closely with results from the full-potential linearized augmented plane-wave implementation. The work attempts to overcome the uncertainties inherent in earlier DFT calculations of the mel"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0706.1012","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0706.1012/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"0706.1012","created_at":"2026-07-04T17:04:06.953831+00:00"},{"alias_kind":"arxiv_version","alias_value":"0706.1012v1","created_at":"2026-07-04T17:04:06.953831+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0706.1012","created_at":"2026-07-04T17:04:06.953831+00:00"},{"alias_kind":"pith_short_12","alias_value":"YXIRUWD7CBBF","created_at":"2026-07-04T17:04:06.953831+00:00"},{"alias_kind":"pith_short_16","alias_value":"YXIRUWD7CBBFQWXK","created_at":"2026-07-04T17:04:06.953831+00:00"},{"alias_kind":"pith_short_8","alias_value":"YXIRUWD7","created_at":"2026-07-04T17:04:06.953831+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.04973","citing_title":"SLUSCHI-UP: A Web Infrastructure for SLUSCHI Melting-Temperature Calculations Using Universal Machine-Learning Interatomic Potentials","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX","json":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX.json","graph_json":"https://pith.science/api/pith-number/YXIRUWD7CBBFQWXKGYC27CV2UX/graph.json","events_json":"https://pith.science/api/pith-number/YXIRUWD7CBBFQWXKGYC27CV2UX/events.json","paper":"https://pith.science/paper/YXIRUWD7"},"agent_actions":{"view_html":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX","download_json":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX.json","view_paper":"https://pith.science/paper/YXIRUWD7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0706.1012&json=true","fetch_graph":"https://pith.science/api/pith-number/YXIRUWD7CBBFQWXKGYC27CV2UX/graph.json","fetch_events":"https://pith.science/api/pith-number/YXIRUWD7CBBFQWXKGYC27CV2UX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX/action/storage_attestation","attest_author":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX/action/author_attestation","sign_citation":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX/action/citation_signature","submit_replication":"https://pith.science/pith/YXIRUWD7CBBFQWXKGYC27CV2UX/action/replication_record"}},"created_at":"2026-07-04T17:04:06.953831+00:00","updated_at":"2026-07-04T17:04:06.953831+00:00"}