{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:DSJS2LHPYLB7HVMGTNR6EOM44F","short_pith_number":"pith:DSJS2LHP","schema_version":"1.0","canonical_sha256":"1c932d2cefc2c3f3d5869b63e2399ce157f285e1830fceaf033925a5a4841e68","source":{"kind":"arxiv","id":"1205.3301","version":2},"attestation_state":"computed","paper":{"title":"Spin-stripe density varies linearly with hole content in single-layer Bi2201 cuprate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. K. Singh, J. M. Tranquada, K. Yamada, M. Enoki, M. Fujita, S. Chang, S. Iikubo, T. Nishizaki","submitted_at":"2012-05-15T09:24:48Z","abstract_excerpt":"We have performed inelastic neutron scattering measurements on the single-layer cuprate Bi2+xSr2-xCuO6+y (Bi2201) with x=0.2, 0.3, 0.4 and 0.5, a doping range that spans the spin-glass (SG) to superconducting (SC) phase boundary. The doping evolution of low energy spin fluctuations was found to be characterized by a change of incommensurate modulation wave vector from the tetragonal [110] to [100]/[010] directions, while maintaining a linear relation between the incommensurability and the hole concentration, delta p. In the SC regime, the spectral weight is strongly suppressed below 4 meV. Sim"},"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":"1205.3301","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-05-15T09:24:48Z","cross_cats_sorted":[],"title_canon_sha256":"37ee2a01fe0d8f7c3cd13ede798f27b0b1fb89a85e1de61c8d5342cd270f5df4","abstract_canon_sha256":"3b6dbd4b7b61b8655fafaa7aeef992e6d7c9ffabfbfdde50f2b9c244376bf0d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:34:35.543966Z","signature_b64":"vNwdmppS31TfmZIhFiqsn9vq7W7f+0qDxKfbr2ESqliFRKKgj6NLaZp22+3KxRCB99yV+gZdlo2IgOhTFnMcAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c932d2cefc2c3f3d5869b63e2399ce157f285e1830fceaf033925a5a4841e68","last_reissued_at":"2026-05-18T03:34:35.543209Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:34:35.543209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin-stripe density varies linearly with hole content in single-layer Bi2201 cuprate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. K. Singh, J. M. Tranquada, K. Yamada, M. Enoki, M. Fujita, S. Chang, S. Iikubo, T. Nishizaki","submitted_at":"2012-05-15T09:24:48Z","abstract_excerpt":"We have performed inelastic neutron scattering measurements on the single-layer cuprate Bi2+xSr2-xCuO6+y (Bi2201) with x=0.2, 0.3, 0.4 and 0.5, a doping range that spans the spin-glass (SG) to superconducting (SC) phase boundary. The doping evolution of low energy spin fluctuations was found to be characterized by a change of incommensurate modulation wave vector from the tetragonal [110] to [100]/[010] directions, while maintaining a linear relation between the incommensurability and the hole concentration, delta p. In the SC regime, the spectral weight is strongly suppressed below 4 meV. Sim"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.3301","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":"1205.3301","created_at":"2026-05-18T03:34:35.543341+00:00"},{"alias_kind":"arxiv_version","alias_value":"1205.3301v2","created_at":"2026-05-18T03:34:35.543341+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.3301","created_at":"2026-05-18T03:34:35.543341+00:00"},{"alias_kind":"pith_short_12","alias_value":"DSJS2LHPYLB7","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"DSJS2LHPYLB7HVMG","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"DSJS2LHP","created_at":"2026-05-18T12:27:04.183437+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/DSJS2LHPYLB7HVMGTNR6EOM44F","json":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F.json","graph_json":"https://pith.science/api/pith-number/DSJS2LHPYLB7HVMGTNR6EOM44F/graph.json","events_json":"https://pith.science/api/pith-number/DSJS2LHPYLB7HVMGTNR6EOM44F/events.json","paper":"https://pith.science/paper/DSJS2LHP"},"agent_actions":{"view_html":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F","download_json":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F.json","view_paper":"https://pith.science/paper/DSJS2LHP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1205.3301&json=true","fetch_graph":"https://pith.science/api/pith-number/DSJS2LHPYLB7HVMGTNR6EOM44F/graph.json","fetch_events":"https://pith.science/api/pith-number/DSJS2LHPYLB7HVMGTNR6EOM44F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F/action/storage_attestation","attest_author":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F/action/author_attestation","sign_citation":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F/action/citation_signature","submit_replication":"https://pith.science/pith/DSJS2LHPYLB7HVMGTNR6EOM44F/action/replication_record"}},"created_at":"2026-05-18T03:34:35.543341+00:00","updated_at":"2026-05-18T03:34:35.543341+00:00"}