{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WHJS2FLJ22NYOFEORAK3UAHJME","short_pith_number":"pith:WHJS2FLJ","schema_version":"1.0","canonical_sha256":"b1d32d1569d69b87148e8815ba00e9613a550201ccecaf86b5540c91e997ab66","source":{"kind":"arxiv","id":"2410.18747","version":2},"attestation_state":"computed","paper":{"title":"Monopole excitations in the $U(1)$ Dirac spin liquid on the triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alberto Parola, Didier Poilblanc, Federico Becca, Sasank Budaraju, Yasir Iqbal","submitted_at":"2024-10-24T13:53:46Z","abstract_excerpt":"The $U(1)$ Dirac spin liquid might realize an exotic phase of matter whose low-energy properties are described by quantum electrodynamics in $2+1$ dimensions, where gapless modes exists but spinons and gauge fields are strongly coupled. Its existence has been proposed in frustrated Heisenberg models in presence of frustrating super-exchange interactions, by the (Abrikosov) fermionic representation of the spin operators [X.-G. Wen, \\href{https://doi.org/10.1103/PhysRevB.65.165113}{Phys. Rev. B {\\bf 65}, 165113 (2002)}], supplemented by the Gutzwiller projection. Here, we construct charge-$Q$ mo"},"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":"2410.18747","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-10-24T13:53:46Z","cross_cats_sorted":[],"title_canon_sha256":"ba76c6ab0b33cc7dab4c92ccda08c40d42a484dac7d3f1f6d2d5450174470232","abstract_canon_sha256":"0a79918fd033df7851a9f6b859f912c89048fff077b9ecfe739951f801168d0c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:40:13.774439Z","signature_b64":"h8Kxf5/trPzJdjo0VeIPz1GqnP25QBOlxl2KnSHW06HaMb2mCjn+piDS7TCx+WHwU/M9F9XsKdI1f8QVw6LJAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1d32d1569d69b87148e8815ba00e9613a550201ccecaf86b5540c91e997ab66","last_reissued_at":"2026-07-05T10:40:13.773976Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:40:13.773976Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Monopole excitations in the $U(1)$ Dirac spin liquid on the triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alberto Parola, Didier Poilblanc, Federico Becca, Sasank Budaraju, Yasir Iqbal","submitted_at":"2024-10-24T13:53:46Z","abstract_excerpt":"The $U(1)$ Dirac spin liquid might realize an exotic phase of matter whose low-energy properties are described by quantum electrodynamics in $2+1$ dimensions, where gapless modes exists but spinons and gauge fields are strongly coupled. Its existence has been proposed in frustrated Heisenberg models in presence of frustrating super-exchange interactions, by the (Abrikosov) fermionic representation of the spin operators [X.-G. Wen, \\href{https://doi.org/10.1103/PhysRevB.65.165113}{Phys. Rev. B {\\bf 65}, 165113 (2002)}], supplemented by the Gutzwiller projection. Here, we construct charge-$Q$ mo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.18747","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/2410.18747/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":"2410.18747","created_at":"2026-07-05T10:40:13.774034+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.18747v2","created_at":"2026-07-05T10:40:13.774034+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.18747","created_at":"2026-07-05T10:40:13.774034+00:00"},{"alias_kind":"pith_short_12","alias_value":"WHJS2FLJ22NY","created_at":"2026-07-05T10:40:13.774034+00:00"},{"alias_kind":"pith_short_16","alias_value":"WHJS2FLJ22NYOFEO","created_at":"2026-07-05T10:40:13.774034+00:00"},{"alias_kind":"pith_short_8","alias_value":"WHJS2FLJ","created_at":"2026-07-05T10:40:13.774034+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2503.07689","citing_title":"Quantum phase diagram of the spin-$\\frac{1}{2}$ Heisenberg antiferromagnet on the square-kagome lattice: a tensor network study","ref_index":51,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME","json":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME.json","graph_json":"https://pith.science/api/pith-number/WHJS2FLJ22NYOFEORAK3UAHJME/graph.json","events_json":"https://pith.science/api/pith-number/WHJS2FLJ22NYOFEORAK3UAHJME/events.json","paper":"https://pith.science/paper/WHJS2FLJ"},"agent_actions":{"view_html":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME","download_json":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME.json","view_paper":"https://pith.science/paper/WHJS2FLJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.18747&json=true","fetch_graph":"https://pith.science/api/pith-number/WHJS2FLJ22NYOFEORAK3UAHJME/graph.json","fetch_events":"https://pith.science/api/pith-number/WHJS2FLJ22NYOFEORAK3UAHJME/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME/action/storage_attestation","attest_author":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME/action/author_attestation","sign_citation":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME/action/citation_signature","submit_replication":"https://pith.science/pith/WHJS2FLJ22NYOFEORAK3UAHJME/action/replication_record"}},"created_at":"2026-07-05T10:40:13.774034+00:00","updated_at":"2026-07-05T10:40:13.774034+00:00"}