{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:K7PWAMY6QPPHPC2I6CWIVVVNOL","short_pith_number":"pith:K7PWAMY6","schema_version":"1.0","canonical_sha256":"57df60331e83de778b48f0ac8ad6ad72c0b40f5334c3219f83d47130b0f4bbe9","source":{"kind":"arxiv","id":"1707.00068","version":2},"attestation_state":"computed","paper":{"title":"Intrinsic translational symmetry breaking in a doped Mott insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. N. Sheng, Zheng-Yu Weng, Zheng Zhu","submitted_at":"2017-07-01T00:06:57Z","abstract_excerpt":"A central issue of Mott physics, with symmetries being fully retained in the spin background, concerns the charge excitation. In a two-leg spin ladder with spin gap, an injected hole can exhibit either a Bloch wave or a density wave by tuning the ladder anisotropy through a `quantum critical point' (QCP). The nature of such a QCP has been a subject of recent studies by density matrix renormalization group (DMRG). In this paper, we reexamine the ground state of the one doped hole, and show that a two-component structure is present in the density wave regime in contrast to the single component i"},"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":"1707.00068","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-07-01T00:06:57Z","cross_cats_sorted":[],"title_canon_sha256":"1e23e4d914a8351339e3426d60b8b81d4db6a4e35b1c8dc3ae3db352bf02cdf9","abstract_canon_sha256":"ed523229ee0bfe1c3c020874201169cb61fa2034ddc1180b8e73d7fb302f7241"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:04.174775Z","signature_b64":"R2CZfpCKRKhMrfdymyFGk55ZL1vNpz1jNQHmmui6HCjhDZtM+3yCdpgU6UwY8S77Z23/a1W5yqG4m4ALzasQDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57df60331e83de778b48f0ac8ad6ad72c0b40f5334c3219f83d47130b0f4bbe9","last_reissued_at":"2026-05-18T00:10:04.174052Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:04.174052Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Intrinsic translational symmetry breaking in a doped Mott insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. N. Sheng, Zheng-Yu Weng, Zheng Zhu","submitted_at":"2017-07-01T00:06:57Z","abstract_excerpt":"A central issue of Mott physics, with symmetries being fully retained in the spin background, concerns the charge excitation. In a two-leg spin ladder with spin gap, an injected hole can exhibit either a Bloch wave or a density wave by tuning the ladder anisotropy through a `quantum critical point' (QCP). The nature of such a QCP has been a subject of recent studies by density matrix renormalization group (DMRG). In this paper, we reexamine the ground state of the one doped hole, and show that a two-component structure is present in the density wave regime in contrast to the single component i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.00068","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":"1707.00068","created_at":"2026-05-18T00:10:04.174169+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.00068v2","created_at":"2026-05-18T00:10:04.174169+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.00068","created_at":"2026-05-18T00:10:04.174169+00:00"},{"alias_kind":"pith_short_12","alias_value":"K7PWAMY6QPPH","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"K7PWAMY6QPPHPC2I","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"K7PWAMY6","created_at":"2026-05-18T12:31:24.725408+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/K7PWAMY6QPPHPC2I6CWIVVVNOL","json":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL.json","graph_json":"https://pith.science/api/pith-number/K7PWAMY6QPPHPC2I6CWIVVVNOL/graph.json","events_json":"https://pith.science/api/pith-number/K7PWAMY6QPPHPC2I6CWIVVVNOL/events.json","paper":"https://pith.science/paper/K7PWAMY6"},"agent_actions":{"view_html":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL","download_json":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL.json","view_paper":"https://pith.science/paper/K7PWAMY6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.00068&json=true","fetch_graph":"https://pith.science/api/pith-number/K7PWAMY6QPPHPC2I6CWIVVVNOL/graph.json","fetch_events":"https://pith.science/api/pith-number/K7PWAMY6QPPHPC2I6CWIVVVNOL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL/action/storage_attestation","attest_author":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL/action/author_attestation","sign_citation":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL/action/citation_signature","submit_replication":"https://pith.science/pith/K7PWAMY6QPPHPC2I6CWIVVVNOL/action/replication_record"}},"created_at":"2026-05-18T00:10:04.174169+00:00","updated_at":"2026-05-18T00:10:04.174169+00:00"}