{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:KNAGAUSVHZ5G2CIK6IGQTGPEEV","short_pith_number":"pith:KNAGAUSV","schema_version":"1.0","canonical_sha256":"53406052553e7a6d090af20d0999e4257fa505c8e3730c6be070bbd8f14f25b2","source":{"kind":"arxiv","id":"0903.3137","version":1},"attestation_state":"computed","paper":{"title":"Field Reentrance of the Hidden Order State of URu2Si2 under Pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Atsushi Miyake, Dai Aoki, Elena Hassinger, Frederic Bourdarot, Georg Knebel, Jacques Flouquet, Stephane Raymond, Valentin Taufour","submitted_at":"2009-03-18T11:27:26Z","abstract_excerpt":"Combination of neutron scattering and thermal expansion measurements under pressure shows that the so-called hidden order phase of URu2Si2 reenters in magnetic field when antiferromagnetism (AF) collapses at H_AF (T). Macroscopic pressure studies of the HO-AF boundaries were realized at different pressures via thermal expansion measurements under magnetic field using a strain gauge. Microscopic proof at a given pressure is the reappearance of the resonance at Q_0=(1,0,0) under field which is correlated with the collapse of the AF Bragg reflections at Q_0."},"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":"0903.3137","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2009-03-18T11:27:26Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"e4774129dc325fe5f69c5069c2c99462f2bf9d4d3497bce0980f9dd378a0c415","abstract_canon_sha256":"08aff4e82cb977e4830106f905ebb8abd256d344507c2391bdc000dbff056f27"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:14:46.317277Z","signature_b64":"cW6TVGj3gYplY05hRk/UcOk2eNMeZJc1GSB54ut9WOjkf0TYbliOffJ1M5aqyTmqyNXFAdAe68QqUvIPkmDpCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53406052553e7a6d090af20d0999e4257fa505c8e3730c6be070bbd8f14f25b2","last_reissued_at":"2026-05-18T04:14:46.316609Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:14:46.316609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Field Reentrance of the Hidden Order State of URu2Si2 under Pressure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Atsushi Miyake, Dai Aoki, Elena Hassinger, Frederic Bourdarot, Georg Knebel, Jacques Flouquet, Stephane Raymond, Valentin Taufour","submitted_at":"2009-03-18T11:27:26Z","abstract_excerpt":"Combination of neutron scattering and thermal expansion measurements under pressure shows that the so-called hidden order phase of URu2Si2 reenters in magnetic field when antiferromagnetism (AF) collapses at H_AF (T). Macroscopic pressure studies of the HO-AF boundaries were realized at different pressures via thermal expansion measurements under magnetic field using a strain gauge. Microscopic proof at a given pressure is the reappearance of the resonance at Q_0=(1,0,0) under field which is correlated with the collapse of the AF Bragg reflections at Q_0."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.3137","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":""},"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":"0903.3137","created_at":"2026-05-18T04:14:46.316702+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.3137v1","created_at":"2026-05-18T04:14:46.316702+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.3137","created_at":"2026-05-18T04:14:46.316702+00:00"},{"alias_kind":"pith_short_12","alias_value":"KNAGAUSVHZ5G","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"KNAGAUSVHZ5G2CIK","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"KNAGAUSV","created_at":"2026-05-18T12:26:00.592388+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/KNAGAUSVHZ5G2CIK6IGQTGPEEV","json":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV.json","graph_json":"https://pith.science/api/pith-number/KNAGAUSVHZ5G2CIK6IGQTGPEEV/graph.json","events_json":"https://pith.science/api/pith-number/KNAGAUSVHZ5G2CIK6IGQTGPEEV/events.json","paper":"https://pith.science/paper/KNAGAUSV"},"agent_actions":{"view_html":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV","download_json":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV.json","view_paper":"https://pith.science/paper/KNAGAUSV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.3137&json=true","fetch_graph":"https://pith.science/api/pith-number/KNAGAUSVHZ5G2CIK6IGQTGPEEV/graph.json","fetch_events":"https://pith.science/api/pith-number/KNAGAUSVHZ5G2CIK6IGQTGPEEV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV/action/storage_attestation","attest_author":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV/action/author_attestation","sign_citation":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV/action/citation_signature","submit_replication":"https://pith.science/pith/KNAGAUSVHZ5G2CIK6IGQTGPEEV/action/replication_record"}},"created_at":"2026-05-18T04:14:46.316702+00:00","updated_at":"2026-05-18T04:14:46.316702+00:00"}