{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:FL2267MCUUDGEH2LW5Q2PK7A2J","short_pith_number":"pith:FL2267MC","schema_version":"1.0","canonical_sha256":"2af5af7d82a506621f4bb761a7abe0d25681a555c9fd56541e41b751d3921963","source":{"kind":"arxiv","id":"1610.00435","version":1},"attestation_state":"computed","paper":{"title":"Thallium under extreme compression","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.chem-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Cazorla, C. Popescu, D. Errandonea, K. A. Munro, M. I. McMahon, S. G. MacLeod","submitted_at":"2016-10-03T07:50:24Z","abstract_excerpt":"We present a combined theoretical and experimental study of the high-pressure behavior of thallium. X-ray diffraction experiments have been carried out at room temperature up to 125 GPa using diamond-anvil cells, nearly doubling the pressure range of previous experiments. We have confirmed the hcp-fcc transition at 3.5 GPa and determined that the fcc structure remains stable up to the highest pressure attained in the experiments. In addition, HP-HT experiments have been performed up to 8 GPa and 700 K by using a combination of x-ray diffraction and a resistively heated diamond-anvil cell. Info"},"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":"1610.00435","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2016-10-03T07:50:24Z","cross_cats_sorted":["cond-mat.other","physics.chem-ph"],"title_canon_sha256":"68f0e9697f911be0c7eb7f5da26a9ed6c0a09442914d8833f0204f3c3c6aa6e2","abstract_canon_sha256":"1c191c586fb5977c43068c974948407c00231fccf5d92049b091b4f9fa2ab8d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:25.538285Z","signature_b64":"D3cSXwaR3XXz5glY4iWaCYC7zIast5s72k3XirrUYi8U6ur2LrY2x1dGMCSQOEsey0jXxAxKpzPqf1vbH7BjDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2af5af7d82a506621f4bb761a7abe0d25681a555c9fd56541e41b751d3921963","last_reissued_at":"2026-05-18T01:03:25.537790Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:25.537790Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thallium under extreme compression","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.chem-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Cazorla, C. Popescu, D. Errandonea, K. A. Munro, M. I. McMahon, S. G. MacLeod","submitted_at":"2016-10-03T07:50:24Z","abstract_excerpt":"We present a combined theoretical and experimental study of the high-pressure behavior of thallium. X-ray diffraction experiments have been carried out at room temperature up to 125 GPa using diamond-anvil cells, nearly doubling the pressure range of previous experiments. We have confirmed the hcp-fcc transition at 3.5 GPa and determined that the fcc structure remains stable up to the highest pressure attained in the experiments. In addition, HP-HT experiments have been performed up to 8 GPa and 700 K by using a combination of x-ray diffraction and a resistively heated diamond-anvil cell. Info"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.00435","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":"1610.00435","created_at":"2026-05-18T01:03:25.537866+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.00435v1","created_at":"2026-05-18T01:03:25.537866+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.00435","created_at":"2026-05-18T01:03:25.537866+00:00"},{"alias_kind":"pith_short_12","alias_value":"FL2267MCUUDG","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"FL2267MCUUDGEH2L","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"FL2267MC","created_at":"2026-05-18T12:30:15.759754+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/FL2267MCUUDGEH2LW5Q2PK7A2J","json":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J.json","graph_json":"https://pith.science/api/pith-number/FL2267MCUUDGEH2LW5Q2PK7A2J/graph.json","events_json":"https://pith.science/api/pith-number/FL2267MCUUDGEH2LW5Q2PK7A2J/events.json","paper":"https://pith.science/paper/FL2267MC"},"agent_actions":{"view_html":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J","download_json":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J.json","view_paper":"https://pith.science/paper/FL2267MC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.00435&json=true","fetch_graph":"https://pith.science/api/pith-number/FL2267MCUUDGEH2LW5Q2PK7A2J/graph.json","fetch_events":"https://pith.science/api/pith-number/FL2267MCUUDGEH2LW5Q2PK7A2J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J/action/storage_attestation","attest_author":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J/action/author_attestation","sign_citation":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J/action/citation_signature","submit_replication":"https://pith.science/pith/FL2267MCUUDGEH2LW5Q2PK7A2J/action/replication_record"}},"created_at":"2026-05-18T01:03:25.537866+00:00","updated_at":"2026-05-18T01:03:25.537866+00:00"}