{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:JTTRNXG7LXIRFI2EJSWITKD47B","short_pith_number":"pith:JTTRNXG7","schema_version":"1.0","canonical_sha256":"4ce716dcdf5dd112a3444cac89a87cf8569a1e211f0fd5edc4efc1e886bfb71c","source":{"kind":"arxiv","id":"2211.08823","version":2},"attestation_state":"computed","paper":{"title":"Classical and quantum phases of the pyrochlore $S=1/2$ magnet with Heisenberg and Dzyaloshinskii-Moriya interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Daniel Lozano-G\\'omez, Jaan Oitmaa, Johannes Reuther, Michel J. P. Gingras, Rajiv R. P. Singh, Vincent Noculak, Yasir Iqbal","submitted_at":"2022-11-16T10:48:13Z","abstract_excerpt":"We investigate the ground state and critical temperature phase diagrams of the classical and quantum $S=1/2$ pyrochlore lattice with nearest-neighbor Heisenberg and Dzyaloshinskii-Moriya interactions (DMI). We consider ferromagnetic and antiferromagnetic Heisenberg exchange as well as direct and indirect DMI. Classically, three ground states are found: all-in/all-out, ferromagnetic and a locally ordered $XY$ phase, known as $\\Gamma_5$, which displays an accidental classical U(1) degeneracy. Quantum zero-point energy fluctuations are found to lift the classical ground state degeneracy and selec"},"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":"2211.08823","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-11-16T10:48:13Z","cross_cats_sorted":[],"title_canon_sha256":"dca36d4af2d47dfd9263dfeec2a34ca1f8f261853f7787f16863880e6c9f38c7","abstract_canon_sha256":"63b2e924b1ea45c5b3117d41c66f113c35276ffff9fbed0c59cd67e43bbdd0bf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:21:55.180358Z","signature_b64":"UUAb98BQIGaaWnD54xzJ4QG7sW4N7EFc0R58xFGwI1jMsNf9qOsk3yzUvyUSLHsUno8HnCGPnDORQf23r6HCDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ce716dcdf5dd112a3444cac89a87cf8569a1e211f0fd5edc4efc1e886bfb71c","last_reissued_at":"2026-07-05T06:21:55.179793Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:21:55.179793Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Classical and quantum phases of the pyrochlore $S=1/2$ magnet with Heisenberg and Dzyaloshinskii-Moriya interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Daniel Lozano-G\\'omez, Jaan Oitmaa, Johannes Reuther, Michel J. P. Gingras, Rajiv R. P. Singh, Vincent Noculak, Yasir Iqbal","submitted_at":"2022-11-16T10:48:13Z","abstract_excerpt":"We investigate the ground state and critical temperature phase diagrams of the classical and quantum $S=1/2$ pyrochlore lattice with nearest-neighbor Heisenberg and Dzyaloshinskii-Moriya interactions (DMI). We consider ferromagnetic and antiferromagnetic Heisenberg exchange as well as direct and indirect DMI. Classically, three ground states are found: all-in/all-out, ferromagnetic and a locally ordered $XY$ phase, known as $\\Gamma_5$, which displays an accidental classical U(1) degeneracy. Quantum zero-point energy fluctuations are found to lift the classical ground state degeneracy and selec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.08823","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2211.08823/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":"2211.08823","created_at":"2026-07-05T06:21:55.179853+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.08823v2","created_at":"2026-07-05T06:21:55.179853+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.08823","created_at":"2026-07-05T06:21:55.179853+00:00"},{"alias_kind":"pith_short_12","alias_value":"JTTRNXG7LXIR","created_at":"2026-07-05T06:21:55.179853+00:00"},{"alias_kind":"pith_short_16","alias_value":"JTTRNXG7LXIRFI2E","created_at":"2026-07-05T06:21:55.179853+00:00"},{"alias_kind":"pith_short_8","alias_value":"JTTRNXG7","created_at":"2026-07-05T06:21:55.179853+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/JTTRNXG7LXIRFI2EJSWITKD47B","json":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B.json","graph_json":"https://pith.science/api/pith-number/JTTRNXG7LXIRFI2EJSWITKD47B/graph.json","events_json":"https://pith.science/api/pith-number/JTTRNXG7LXIRFI2EJSWITKD47B/events.json","paper":"https://pith.science/paper/JTTRNXG7"},"agent_actions":{"view_html":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B","download_json":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B.json","view_paper":"https://pith.science/paper/JTTRNXG7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.08823&json=true","fetch_graph":"https://pith.science/api/pith-number/JTTRNXG7LXIRFI2EJSWITKD47B/graph.json","fetch_events":"https://pith.science/api/pith-number/JTTRNXG7LXIRFI2EJSWITKD47B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B/action/storage_attestation","attest_author":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B/action/author_attestation","sign_citation":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B/action/citation_signature","submit_replication":"https://pith.science/pith/JTTRNXG7LXIRFI2EJSWITKD47B/action/replication_record"}},"created_at":"2026-07-05T06:21:55.179853+00:00","updated_at":"2026-07-05T06:21:55.179853+00:00"}