{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LEHGOXZCE56T3HASP4FPCRKOQ7","short_pith_number":"pith:LEHGOXZC","schema_version":"1.0","canonical_sha256":"590e675f22277d3d9c127f0af1454e87d59b5264abd3c7dcad7919b326a8f6e7","source":{"kind":"arxiv","id":"1401.6586","version":2},"attestation_state":"computed","paper":{"title":"Strong particle-hole asymmetry of charge instabilities in doped Mott insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Andres Greco, Hiroyuki Yamase, Matias Bejas","submitted_at":"2014-01-25T22:17:22Z","abstract_excerpt":"We study possible charge instabilities in doped Mott insulators by employing the two-dimensional t-J model with a positive value of the next nearest-neighbor hopping integral t' on a square lattice, which is applicable to electron-doped cuprates. Although the d-wave charge density wave (flux phase) and d-wave Pomeranchuk instability (nematic order) are dominant instabilities for a negative t' that corresponds to hole-doped cuprates, we find that those instabilities are strongly suppressed and become relevant only rather close to half filling. Instead, various types of bond orders with modulati"},"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":"1401.6586","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-01-25T22:17:22Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"58aae5f9178b66fd9ddb2e1fbacb290949e100c0c6309c7491897b18d8e5e79d","abstract_canon_sha256":"3449c45cdf2b8300364676ec50ea3dcbfbc06a4d8a1603bd632a5a177ceeae03"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:14.227712Z","signature_b64":"bf2RAVfXLLNq/F6yFHhxFjPyWREKnSmJe5X21HKcsYbS4uR0VyCaAQe1y6ZI6xGcCIjyJrzqSH1vHh2he+evBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"590e675f22277d3d9c127f0af1454e87d59b5264abd3c7dcad7919b326a8f6e7","last_reissued_at":"2026-05-18T02:32:14.227079Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:14.227079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong particle-hole asymmetry of charge instabilities in doped Mott insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Andres Greco, Hiroyuki Yamase, Matias Bejas","submitted_at":"2014-01-25T22:17:22Z","abstract_excerpt":"We study possible charge instabilities in doped Mott insulators by employing the two-dimensional t-J model with a positive value of the next nearest-neighbor hopping integral t' on a square lattice, which is applicable to electron-doped cuprates. Although the d-wave charge density wave (flux phase) and d-wave Pomeranchuk instability (nematic order) are dominant instabilities for a negative t' that corresponds to hole-doped cuprates, we find that those instabilities are strongly suppressed and become relevant only rather close to half filling. Instead, various types of bond orders with modulati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.6586","kind":"arxiv","version":2},"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":"1401.6586","created_at":"2026-05-18T02:32:14.227170+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.6586v2","created_at":"2026-05-18T02:32:14.227170+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.6586","created_at":"2026-05-18T02:32:14.227170+00:00"},{"alias_kind":"pith_short_12","alias_value":"LEHGOXZCE56T","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"LEHGOXZCE56T3HAS","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"LEHGOXZC","created_at":"2026-05-18T12:28:38.356838+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/LEHGOXZCE56T3HASP4FPCRKOQ7","json":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7.json","graph_json":"https://pith.science/api/pith-number/LEHGOXZCE56T3HASP4FPCRKOQ7/graph.json","events_json":"https://pith.science/api/pith-number/LEHGOXZCE56T3HASP4FPCRKOQ7/events.json","paper":"https://pith.science/paper/LEHGOXZC"},"agent_actions":{"view_html":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7","download_json":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7.json","view_paper":"https://pith.science/paper/LEHGOXZC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.6586&json=true","fetch_graph":"https://pith.science/api/pith-number/LEHGOXZCE56T3HASP4FPCRKOQ7/graph.json","fetch_events":"https://pith.science/api/pith-number/LEHGOXZCE56T3HASP4FPCRKOQ7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7/action/storage_attestation","attest_author":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7/action/author_attestation","sign_citation":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7/action/citation_signature","submit_replication":"https://pith.science/pith/LEHGOXZCE56T3HASP4FPCRKOQ7/action/replication_record"}},"created_at":"2026-05-18T02:32:14.227170+00:00","updated_at":"2026-05-18T02:32:14.227170+00:00"}