{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:TQMQW54YDLPYDJALWABNDUYPFX","short_pith_number":"pith:TQMQW54Y","schema_version":"1.0","canonical_sha256":"9c190b77981adf81a40bb002d1d30f2dda00727e4fd3af3e5bcb79bb93a79b45","source":{"kind":"arxiv","id":"1805.05547","version":1},"attestation_state":"computed","paper":{"title":"Commensurate vs incommensurate charge ordering near the superconducting dome in Ir$_{1-x}$Pt$_x$Te$_2$ revealed by resonant x-ray scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"F. He, G. Matsuo, H. Ishii, H. Nakao, H. Wadati, K. Ishii, K. Kudo, K. Takubo, K. Yamamoto, M. Kobayashi, M. Nohara, R. Sutarto, T. Mizokawa, Y. Hirata, Y. Murakami, Y. Yamasaki","submitted_at":"2018-05-15T03:24:05Z","abstract_excerpt":"The electronic-structural modulations of Ir$_{1-x}$Pt$_x$Te$_2$ (0 $\\leqq x\\leqq$ 0.12) have been examined by resonant elastic x-ray scattering (REXS) and resonant inelastic x-ray scattering (RIXS) techniques at both the Ir and Te edges. Charge-density-wave-like superstructure with wave vectors of $\\mathbf{Q}$=(1/5 0 $-$1/5), (1/8 0 $-$1/8), and (1/6 0 $-$1/6) are observed on the same sample of IrTe$_2$ at the lowest temperature, the patterns of which are controlled by the cooling speeds. In contrast, superstructures around $\\mathbf{Q}$=(1/5 0 $-$1/5) are observed for doped samples (0.02 $\\leq"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1805.05547","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-05-15T03:24:05Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"57a7e9c123c95efe02e44394ac9087fdffea1a6ace76f4e276763c02ff6ec51f","abstract_canon_sha256":"74c1ea23cea7809984928689a7198e5cf8ce72e1fa617b2a200c893cc0c5d0e2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:33.826026Z","signature_b64":"orPxrzk1qrZ81Vr3ufITSwoEXHe5xjNdY9KhsAT5KcsYtO0jnETJeD4fAx7u/iOTscCNauwAfREg3X2c3WfmCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9c190b77981adf81a40bb002d1d30f2dda00727e4fd3af3e5bcb79bb93a79b45","last_reissued_at":"2026-05-18T00:11:33.825428Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:33.825428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Commensurate vs incommensurate charge ordering near the superconducting dome in Ir$_{1-x}$Pt$_x$Te$_2$ revealed by resonant x-ray scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"F. He, G. Matsuo, H. Ishii, H. Nakao, H. Wadati, K. Ishii, K. Kudo, K. Takubo, K. Yamamoto, M. Kobayashi, M. Nohara, R. Sutarto, T. Mizokawa, Y. Hirata, Y. Murakami, Y. Yamasaki","submitted_at":"2018-05-15T03:24:05Z","abstract_excerpt":"The electronic-structural modulations of Ir$_{1-x}$Pt$_x$Te$_2$ (0 $\\leqq x\\leqq$ 0.12) have been examined by resonant elastic x-ray scattering (REXS) and resonant inelastic x-ray scattering (RIXS) techniques at both the Ir and Te edges. Charge-density-wave-like superstructure with wave vectors of $\\mathbf{Q}$=(1/5 0 $-$1/5), (1/8 0 $-$1/8), and (1/6 0 $-$1/6) are observed on the same sample of IrTe$_2$ at the lowest temperature, the patterns of which are controlled by the cooling speeds. In contrast, superstructures around $\\mathbf{Q}$=(1/5 0 $-$1/5) are observed for doped samples (0.02 $\\leq"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05547","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":"1805.05547","created_at":"2026-05-18T00:11:33.825512+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.05547v1","created_at":"2026-05-18T00:11:33.825512+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.05547","created_at":"2026-05-18T00:11:33.825512+00:00"},{"alias_kind":"pith_short_12","alias_value":"TQMQW54YDLPY","created_at":"2026-05-18T12:32:56.356000+00:00"},{"alias_kind":"pith_short_16","alias_value":"TQMQW54YDLPYDJAL","created_at":"2026-05-18T12:32:56.356000+00:00"},{"alias_kind":"pith_short_8","alias_value":"TQMQW54Y","created_at":"2026-05-18T12:32:56.356000+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/TQMQW54YDLPYDJALWABNDUYPFX","json":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX.json","graph_json":"https://pith.science/api/pith-number/TQMQW54YDLPYDJALWABNDUYPFX/graph.json","events_json":"https://pith.science/api/pith-number/TQMQW54YDLPYDJALWABNDUYPFX/events.json","paper":"https://pith.science/paper/TQMQW54Y"},"agent_actions":{"view_html":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX","download_json":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX.json","view_paper":"https://pith.science/paper/TQMQW54Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.05547&json=true","fetch_graph":"https://pith.science/api/pith-number/TQMQW54YDLPYDJALWABNDUYPFX/graph.json","fetch_events":"https://pith.science/api/pith-number/TQMQW54YDLPYDJALWABNDUYPFX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX/action/storage_attestation","attest_author":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX/action/author_attestation","sign_citation":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX/action/citation_signature","submit_replication":"https://pith.science/pith/TQMQW54YDLPYDJALWABNDUYPFX/action/replication_record"}},"created_at":"2026-05-18T00:11:33.825512+00:00","updated_at":"2026-05-18T00:11:33.825512+00:00"}