{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:FBUEFGVGEAXOAZ2ZJQXMGHPOY6","short_pith_number":"pith:FBUEFGVG","schema_version":"1.0","canonical_sha256":"2868429aa6202ee067594c2ec31deec7bd64b7cb68c524983c1d9d2ec0f480b4","source":{"kind":"arxiv","id":"1709.08998","version":3},"attestation_state":"computed","paper":{"title":"Frustrated spin order and stripe fluctuations in FeSe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Andreas Baum, Brian Moritz, Harrison N. Ruiz, Nenad Lazarevi\\'c, Peter Adelmann, Ramez Hosseinian Ahangharnejhad, Rudi Hackl, Thomas B\\\"ohm, Thomas P. Devereaux, Thomas Wolf, Yao Wang, Zoran V. Popovi\\'c","submitted_at":"2017-09-26T13:18:31Z","abstract_excerpt":"The charge and spin dynamics of the structurally simplest iron-based superconductor, FeSe, may hold the key to understanding the physics of high temperature superconductors in general. Unlike the iron pnictides, FeSe lacks long range magnetic order in spite of a similar structural transition around 90\\,K. Here, we report results of Raman scattering experiments as a function of temperature and polarization and simulations based on exact diagonalization of a frustrated spin model. Both experiment and theory find a persistent low energy peak close to 500cm$^{-1}$ in $B_{1g}$ symmetry, which softe"},"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":"1709.08998","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-09-26T13:18:31Z","cross_cats_sorted":[],"title_canon_sha256":"f991d9e2232c568da6b622e08467a464700b45f9b3290198b765017fa5ada929","abstract_canon_sha256":"4f8df347f260dd67b98d7b21f629e56f0f92f1f142fe0834dbc467cb7c173922"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:03.738104Z","signature_b64":"9p4s7wJ/0EeKdO7xlU4L+1ueUXd+IvjttlPN+noSTYwenKGes6ek5H/zZxumINE0ZnoNWdHGGv/z2cH5rW3sCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2868429aa6202ee067594c2ec31deec7bd64b7cb68c524983c1d9d2ec0f480b4","last_reissued_at":"2026-05-17T23:47:03.737422Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:03.737422Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Frustrated spin order and stripe fluctuations in FeSe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Andreas Baum, Brian Moritz, Harrison N. Ruiz, Nenad Lazarevi\\'c, Peter Adelmann, Ramez Hosseinian Ahangharnejhad, Rudi Hackl, Thomas B\\\"ohm, Thomas P. Devereaux, Thomas Wolf, Yao Wang, Zoran V. Popovi\\'c","submitted_at":"2017-09-26T13:18:31Z","abstract_excerpt":"The charge and spin dynamics of the structurally simplest iron-based superconductor, FeSe, may hold the key to understanding the physics of high temperature superconductors in general. Unlike the iron pnictides, FeSe lacks long range magnetic order in spite of a similar structural transition around 90\\,K. Here, we report results of Raman scattering experiments as a function of temperature and polarization and simulations based on exact diagonalization of a frustrated spin model. Both experiment and theory find a persistent low energy peak close to 500cm$^{-1}$ in $B_{1g}$ symmetry, which softe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.08998","kind":"arxiv","version":3},"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":"1709.08998","created_at":"2026-05-17T23:47:03.737535+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.08998v3","created_at":"2026-05-17T23:47:03.737535+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.08998","created_at":"2026-05-17T23:47:03.737535+00:00"},{"alias_kind":"pith_short_12","alias_value":"FBUEFGVGEAXO","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_16","alias_value":"FBUEFGVGEAXOAZ2Z","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_8","alias_value":"FBUEFGVG","created_at":"2026-05-18T12:31:15.632608+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/FBUEFGVGEAXOAZ2ZJQXMGHPOY6","json":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6.json","graph_json":"https://pith.science/api/pith-number/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/graph.json","events_json":"https://pith.science/api/pith-number/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/events.json","paper":"https://pith.science/paper/FBUEFGVG"},"agent_actions":{"view_html":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6","download_json":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6.json","view_paper":"https://pith.science/paper/FBUEFGVG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.08998&json=true","fetch_graph":"https://pith.science/api/pith-number/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/graph.json","fetch_events":"https://pith.science/api/pith-number/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/action/storage_attestation","attest_author":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/action/author_attestation","sign_citation":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/action/citation_signature","submit_replication":"https://pith.science/pith/FBUEFGVGEAXOAZ2ZJQXMGHPOY6/action/replication_record"}},"created_at":"2026-05-17T23:47:03.737535+00:00","updated_at":"2026-05-17T23:47:03.737535+00:00"}