{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:VTK5MBJ64BGO6NJ2JL3T342DR6","short_pith_number":"pith:VTK5MBJ6","schema_version":"1.0","canonical_sha256":"acd5d6053ee04cef353a4af73df3438fa88539112bd83d9ff94549060d8dd827","source":{"kind":"arxiv","id":"2605.23133","version":1},"attestation_state":"computed","paper":{"title":"Tuning J$_1$-J$_2$ in Quasi-2D Triangular Lattice Antiferromagnet $\\alpha$-SrCr$_2$O$_4$ via Uniaxial Pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chris Lygouras, Jazzmin Victorin, Natalia Drichko, Seyed Koohpayeh, Shreenanda Ghosh","submitted_at":"2026-05-22T01:15:26Z","abstract_excerpt":"Triangular lattice antiferromagnets first attracted attention as a frustrated magnetic lattice which can serve as a platform to realize the resonating valence bond state. While the triangular lattice itself was shown to support classical 120 degree order, many theoretical phase diagrams suggest a quantum spin liquid state within a small range of parameters. One possible avenue to achieve such a state is to tune the anisotropy of the triangular lattice antiferromagnet by applying uniaxial pressure. This motivated our Raman scattering study of quasi-two-dimensional antiferromagnet $\\alpha$-SrCr$"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2605.23133","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-05-22T01:15:26Z","cross_cats_sorted":[],"title_canon_sha256":"c7d3e225b501ab588c201b2ed257eb21f15a0c5ed7ae52fb8146ba265b99b9f6","abstract_canon_sha256":"8ab48e0e3144ba2f0314e105c516018aa602f7a5b64b401d2b63cdb310fd556a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-25T02:01:39.696393Z","signature_b64":"Z4nBI5GpLIgyRe1IDREIUntfqVIay9y4xpbCGNS2xA/ftRxl8FmAmmvyTgeVfBmdv4l4yeF3qWdIUfPH1SFbBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"acd5d6053ee04cef353a4af73df3438fa88539112bd83d9ff94549060d8dd827","last_reissued_at":"2026-05-25T02:01:39.695895Z","signature_status":"signed_v1","first_computed_at":"2026-05-25T02:01:39.695895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning J$_1$-J$_2$ in Quasi-2D Triangular Lattice Antiferromagnet $\\alpha$-SrCr$_2$O$_4$ via Uniaxial Pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chris Lygouras, Jazzmin Victorin, Natalia Drichko, Seyed Koohpayeh, Shreenanda Ghosh","submitted_at":"2026-05-22T01:15:26Z","abstract_excerpt":"Triangular lattice antiferromagnets first attracted attention as a frustrated magnetic lattice which can serve as a platform to realize the resonating valence bond state. While the triangular lattice itself was shown to support classical 120 degree order, many theoretical phase diagrams suggest a quantum spin liquid state within a small range of parameters. One possible avenue to achieve such a state is to tune the anisotropy of the triangular lattice antiferromagnet by applying uniaxial pressure. This motivated our Raman scattering study of quasi-two-dimensional antiferromagnet $\\alpha$-SrCr$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.23133","kind":"arxiv","version":1},"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/2605.23133/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":"2605.23133","created_at":"2026-05-25T02:01:39.695970+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.23133v1","created_at":"2026-05-25T02:01:39.695970+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.23133","created_at":"2026-05-25T02:01:39.695970+00:00"},{"alias_kind":"pith_short_12","alias_value":"VTK5MBJ64BGO","created_at":"2026-05-25T02:01:39.695970+00:00"},{"alias_kind":"pith_short_16","alias_value":"VTK5MBJ64BGO6NJ2","created_at":"2026-05-25T02:01:39.695970+00:00"},{"alias_kind":"pith_short_8","alias_value":"VTK5MBJ6","created_at":"2026-05-25T02:01:39.695970+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/VTK5MBJ64BGO6NJ2JL3T342DR6","json":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6.json","graph_json":"https://pith.science/api/pith-number/VTK5MBJ64BGO6NJ2JL3T342DR6/graph.json","events_json":"https://pith.science/api/pith-number/VTK5MBJ64BGO6NJ2JL3T342DR6/events.json","paper":"https://pith.science/paper/VTK5MBJ6"},"agent_actions":{"view_html":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6","download_json":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6.json","view_paper":"https://pith.science/paper/VTK5MBJ6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.23133&json=true","fetch_graph":"https://pith.science/api/pith-number/VTK5MBJ64BGO6NJ2JL3T342DR6/graph.json","fetch_events":"https://pith.science/api/pith-number/VTK5MBJ64BGO6NJ2JL3T342DR6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6/action/storage_attestation","attest_author":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6/action/author_attestation","sign_citation":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6/action/citation_signature","submit_replication":"https://pith.science/pith/VTK5MBJ64BGO6NJ2JL3T342DR6/action/replication_record"}},"created_at":"2026-05-25T02:01:39.695970+00:00","updated_at":"2026-05-25T02:01:39.695970+00:00"}