{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:VBBCOTVDGPOMCAZQZXDMU4UOH6","short_pith_number":"pith:VBBCOTVD","schema_version":"1.0","canonical_sha256":"a842274ea333dcc10330cdc6ca728e3fa5402670b9dece8a8f33c0fb464170aa","source":{"kind":"arxiv","id":"1305.4042","version":2},"attestation_state":"computed","paper":{"title":"Ghost modes and continuum scattering in the dimerized distorted kagome lattice antiferromagnet Rb$_2$Cu$_3$SnF$_{12}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Podlesnyak, C. Broholm, G. Ehlers, H. Tanaka, K. Matan, T. J. Sato, T. Ono, Y. Fukumoto, Y. Nambu, Y. Zhao","submitted_at":"2013-05-17T10:33:15Z","abstract_excerpt":"High intensity pulsed neutron scattering reveals a new set of magnetic excitations in the pinwheel valence bond solid state of the distorted kagome lattice antiferromagnet Rb$_2$Cu$_3$SnF$_{12}$. The polarization of the dominant dispersive modes (2 meV $<\\hbar\\omega< $7 meV) is determined and found consistent with a dimer series expansion with strong Dzyaloshinskii-Moriya interactions ($D/J=0.18$). A weakly dispersive mode near 5 meV and shifted \"ghosts\" of the main modes are attributed to the enlarged unit cell below a $T=215$ K structural transition. Continuum scattering between 8 meV and 10"},"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":"1305.4042","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-05-17T10:33:15Z","cross_cats_sorted":[],"title_canon_sha256":"b363408c0729cdbbfeb8f1ee495e3aca4c25a00e2300983aa64bdaed6cc105df","abstract_canon_sha256":"761b9f4ea31d9c747bb087e38e52cd7e151fb884a107ddb7a47ff5b406702dc4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:01:33.380468Z","signature_b64":"RVPbG2IFTrKYvFvvMEdstB4EUCAZM8m3a7a6EfjTqUOLYn2nkNz5NxnfQRU/IbAMJnY+6U6E+es0mUSMA9v2Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a842274ea333dcc10330cdc6ca728e3fa5402670b9dece8a8f33c0fb464170aa","last_reissued_at":"2026-05-18T03:01:33.380001Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:01:33.380001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ghost modes and continuum scattering in the dimerized distorted kagome lattice antiferromagnet Rb$_2$Cu$_3$SnF$_{12}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Podlesnyak, C. Broholm, G. Ehlers, H. Tanaka, K. Matan, T. J. Sato, T. Ono, Y. Fukumoto, Y. Nambu, Y. Zhao","submitted_at":"2013-05-17T10:33:15Z","abstract_excerpt":"High intensity pulsed neutron scattering reveals a new set of magnetic excitations in the pinwheel valence bond solid state of the distorted kagome lattice antiferromagnet Rb$_2$Cu$_3$SnF$_{12}$. The polarization of the dominant dispersive modes (2 meV $<\\hbar\\omega< $7 meV) is determined and found consistent with a dimer series expansion with strong Dzyaloshinskii-Moriya interactions ($D/J=0.18$). A weakly dispersive mode near 5 meV and shifted \"ghosts\" of the main modes are attributed to the enlarged unit cell below a $T=215$ K structural transition. Continuum scattering between 8 meV and 10"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.4042","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":""},"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":"1305.4042","created_at":"2026-05-18T03:01:33.380070+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.4042v2","created_at":"2026-05-18T03:01:33.380070+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.4042","created_at":"2026-05-18T03:01:33.380070+00:00"},{"alias_kind":"pith_short_12","alias_value":"VBBCOTVDGPOM","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"VBBCOTVDGPOMCAZQ","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"VBBCOTVD","created_at":"2026-05-18T12:28:04.890932+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/VBBCOTVDGPOMCAZQZXDMU4UOH6","json":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6.json","graph_json":"https://pith.science/api/pith-number/VBBCOTVDGPOMCAZQZXDMU4UOH6/graph.json","events_json":"https://pith.science/api/pith-number/VBBCOTVDGPOMCAZQZXDMU4UOH6/events.json","paper":"https://pith.science/paper/VBBCOTVD"},"agent_actions":{"view_html":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6","download_json":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6.json","view_paper":"https://pith.science/paper/VBBCOTVD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.4042&json=true","fetch_graph":"https://pith.science/api/pith-number/VBBCOTVDGPOMCAZQZXDMU4UOH6/graph.json","fetch_events":"https://pith.science/api/pith-number/VBBCOTVDGPOMCAZQZXDMU4UOH6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6/action/storage_attestation","attest_author":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6/action/author_attestation","sign_citation":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6/action/citation_signature","submit_replication":"https://pith.science/pith/VBBCOTVDGPOMCAZQZXDMU4UOH6/action/replication_record"}},"created_at":"2026-05-18T03:01:33.380070+00:00","updated_at":"2026-05-18T03:01:33.380070+00:00"}