{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:QVRFUJ4RPELUDLCNGUJOTXHKZ7","short_pith_number":"pith:QVRFUJ4R","schema_version":"1.0","canonical_sha256":"85625a2791791741ac4d3512e9dceacffa93194caadca82b40e7693635e2892d","source":{"kind":"arxiv","id":"2311.16889","version":4},"attestation_state":"computed","paper":{"title":"Transformer Wave Function for two dimensional frustrated magnets: emergence of a Spin-Liquid Phase in the Shastry-Sutherland Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.str-el","authors_text":"Alberto Parola, Federico Becca, Luciano Loris Viteritti, Riccardo Rende, Sebastian Goldt","submitted_at":"2023-11-28T15:39:54Z","abstract_excerpt":"Understanding quantum magnetism in two-dimensional systems represents a lively branch in modern condensed-matter physics. In the presence of competing super-exchange couplings, magnetic order is frustrated and can be suppressed down to zero temperature. Still, capturing the correct nature of the exact ground state is a highly complicated task, since energy gaps in the spectrum may be very small and states with different physical properties may have competing energies. Here, we introduce a variational Ansatz for two-dimensional frustrated magnets by leveraging the power of representation learni"},"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":"2311.16889","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-11-28T15:39:54Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"6d9187a40f366328541cb823bfb9c38605b2102cf326b6aa34e709a0f9a9e551","abstract_canon_sha256":"93298b51ff36cd97333627e68c2760971382da433af090ea334bf6387bed5e98"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:46:53.158058Z","signature_b64":"2qFHz8ArAjvpU7Tpn7vHD50IW6rFdrgtOCp70G+uCMosnDAFQp4+83vKiSIXjvESq+h7+L4fIGbNbVwcBjULDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"85625a2791791741ac4d3512e9dceacffa93194caadca82b40e7693635e2892d","last_reissued_at":"2026-07-05T10:46:53.157498Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:46:53.157498Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transformer Wave Function for two dimensional frustrated magnets: emergence of a Spin-Liquid Phase in the Shastry-Sutherland Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.str-el","authors_text":"Alberto Parola, Federico Becca, Luciano Loris Viteritti, Riccardo Rende, Sebastian Goldt","submitted_at":"2023-11-28T15:39:54Z","abstract_excerpt":"Understanding quantum magnetism in two-dimensional systems represents a lively branch in modern condensed-matter physics. In the presence of competing super-exchange couplings, magnetic order is frustrated and can be suppressed down to zero temperature. Still, capturing the correct nature of the exact ground state is a highly complicated task, since energy gaps in the spectrum may be very small and states with different physical properties may have competing energies. Here, we introduce a variational Ansatz for two-dimensional frustrated magnets by leveraging the power of representation learni"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.16889","kind":"arxiv","version":4},"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/2311.16889/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":"2311.16889","created_at":"2026-07-05T10:46:53.157558+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.16889v4","created_at":"2026-07-05T10:46:53.157558+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.16889","created_at":"2026-07-05T10:46:53.157558+00:00"},{"alias_kind":"pith_short_12","alias_value":"QVRFUJ4RPELU","created_at":"2026-07-05T10:46:53.157558+00:00"},{"alias_kind":"pith_short_16","alias_value":"QVRFUJ4RPELUDLCN","created_at":"2026-07-05T10:46:53.157558+00:00"},{"alias_kind":"pith_short_8","alias_value":"QVRFUJ4R","created_at":"2026-07-05T10:46:53.157558+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2412.11778","citing_title":"Time-dependent Neural Galerkin Method for Quantum Dynamics","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2502.14091","citing_title":"Quantum spin liquid phase in the Shastry-Sutherland model revealed by high-precision infinite projected entangled-pair states","ref_index":39,"is_internal_anchor":false},{"citing_arxiv_id":"2602.04943","citing_title":"Graph-Theoretic Analysis of Phase Optimization Complexity in Variational Wave Functions for Heisenberg Antiferromagnets","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24337","citing_title":"New non-Euclidean neural quantum states from hyperbolic Lorentz recurrent architectures","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7","json":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7.json","graph_json":"https://pith.science/api/pith-number/QVRFUJ4RPELUDLCNGUJOTXHKZ7/graph.json","events_json":"https://pith.science/api/pith-number/QVRFUJ4RPELUDLCNGUJOTXHKZ7/events.json","paper":"https://pith.science/paper/QVRFUJ4R"},"agent_actions":{"view_html":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7","download_json":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7.json","view_paper":"https://pith.science/paper/QVRFUJ4R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.16889&json=true","fetch_graph":"https://pith.science/api/pith-number/QVRFUJ4RPELUDLCNGUJOTXHKZ7/graph.json","fetch_events":"https://pith.science/api/pith-number/QVRFUJ4RPELUDLCNGUJOTXHKZ7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7/action/storage_attestation","attest_author":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7/action/author_attestation","sign_citation":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7/action/citation_signature","submit_replication":"https://pith.science/pith/QVRFUJ4RPELUDLCNGUJOTXHKZ7/action/replication_record"}},"created_at":"2026-07-05T10:46:53.157558+00:00","updated_at":"2026-07-05T10:46:53.157558+00:00"}