{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:UA5PMU6ZSI65W6IMNHO2ORFO4A","short_pith_number":"pith:UA5PMU6Z","schema_version":"1.0","canonical_sha256":"a03af653d9923ddb790c69dda744aee0110119dd9f1307c3e18f1e9094d8ae56","source":{"kind":"arxiv","id":"2302.07885","version":6},"attestation_state":"computed","paper":{"title":"A model of $d$-wave superconductivity, antiferromagnetism, and charge order on the square lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Henry Shackleton, Maine Christos, Mathias Scheurer, Subir Sachdev, Ya-Hui Zhang, Zhu-Xi Luo","submitted_at":"2023-02-15T19:00:00Z","abstract_excerpt":"Early studies proposed a connection between cuprate superconductivity and fractionalized spin liquid states. But the low temperature phase diagram is dominated by states without fractionalization, with a competition between superconductivity and charge-ordered states which break translational symmetry. Our theory uncovers novel features associated with a particular spin-liquid presumed to underlie the pseudogap metal, and shows that it has multiple nearly-degenerate instabilities to confinement of fractionalized excitations, leading to antiferromagnetism, $d$-wave superconductivity, and/or cha"},"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":"2302.07885","kind":"arxiv","version":6},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-02-15T19:00:00Z","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"title_canon_sha256":"6e184cca73e4dea06a05e83147cc4f7a10ba7aeee3ff4cf76d825900a573cb36","abstract_canon_sha256":"b0cecda7c93bf3b48fbf523ebeeeb86d271b44041686d4aae043786aeecbe815"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:06:59.735965Z","signature_b64":"b5f01l5zfdxOTSRAsnwT/c4ZHFI7DEHM4wATLvHcb6e+ZBi4u9nnjYSBnEhGx2/teLsjHjgGAEVquT2v8IphDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a03af653d9923ddb790c69dda744aee0110119dd9f1307c3e18f1e9094d8ae56","last_reissued_at":"2026-07-05T11:06:59.735496Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:06:59.735496Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A model of $d$-wave superconductivity, antiferromagnetism, and charge order on the square lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Henry Shackleton, Maine Christos, Mathias Scheurer, Subir Sachdev, Ya-Hui Zhang, Zhu-Xi Luo","submitted_at":"2023-02-15T19:00:00Z","abstract_excerpt":"Early studies proposed a connection between cuprate superconductivity and fractionalized spin liquid states. But the low temperature phase diagram is dominated by states without fractionalization, with a competition between superconductivity and charge-ordered states which break translational symmetry. Our theory uncovers novel features associated with a particular spin-liquid presumed to underlie the pseudogap metal, and shows that it has multiple nearly-degenerate instabilities to confinement of fractionalized excitations, leading to antiferromagnetism, $d$-wave superconductivity, and/or cha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.07885","kind":"arxiv","version":6},"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/2302.07885/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":"2302.07885","created_at":"2026-07-05T11:06:59.735554+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.07885v6","created_at":"2026-07-05T11:06:59.735554+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.07885","created_at":"2026-07-05T11:06:59.735554+00:00"},{"alias_kind":"pith_short_12","alias_value":"UA5PMU6ZSI65","created_at":"2026-07-05T11:06:59.735554+00:00"},{"alias_kind":"pith_short_16","alias_value":"UA5PMU6ZSI65W6IM","created_at":"2026-07-05T11:06:59.735554+00:00"},{"alias_kind":"pith_short_8","alias_value":"UA5PMU6Z","created_at":"2026-07-05T11:06:59.735554+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.00762","citing_title":"Deconfined criticality between an antiferromagnetic insulator and a nodal d-wave superconductor: a quantum Monte Carlo study","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2607.00762","citing_title":"Deconfined criticality between an antiferromagnetic insulator and a nodal d-wave superconductor: a quantum Monte Carlo study","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2507.05336","citing_title":"Thermal SU(2) lattice gauge theory for intertwined orders and hole pockets in the cuprates","ref_index":81,"is_internal_anchor":false},{"citing_arxiv_id":"2508.20164","citing_title":"Fractionalized Fermi liquids and the cuprate phase diagram","ref_index":58,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A","json":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A.json","graph_json":"https://pith.science/api/pith-number/UA5PMU6ZSI65W6IMNHO2ORFO4A/graph.json","events_json":"https://pith.science/api/pith-number/UA5PMU6ZSI65W6IMNHO2ORFO4A/events.json","paper":"https://pith.science/paper/UA5PMU6Z"},"agent_actions":{"view_html":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A","download_json":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A.json","view_paper":"https://pith.science/paper/UA5PMU6Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.07885&json=true","fetch_graph":"https://pith.science/api/pith-number/UA5PMU6ZSI65W6IMNHO2ORFO4A/graph.json","fetch_events":"https://pith.science/api/pith-number/UA5PMU6ZSI65W6IMNHO2ORFO4A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A/action/storage_attestation","attest_author":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A/action/author_attestation","sign_citation":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A/action/citation_signature","submit_replication":"https://pith.science/pith/UA5PMU6ZSI65W6IMNHO2ORFO4A/action/replication_record"}},"created_at":"2026-07-05T11:06:59.735554+00:00","updated_at":"2026-07-05T11:06:59.735554+00:00"}