{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:DRK6MC3BBA6PLNO6Y7SHKP2H54","short_pith_number":"pith:DRK6MC3B","schema_version":"1.0","canonical_sha256":"1c55e60b61083cf5b5dec7e4753f47ef0188407eaaa647498c9b0ce7e723b3c8","source":{"kind":"arxiv","id":"1511.02483","version":1},"attestation_state":"computed","paper":{"title":"Quantum phase transitions and decoupling of magnetic sublattices in the quasi-two-dimensional Ising magnet Co3V2O8 in a transverse magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. D. Gaulin, G. Ehlers, H. A. Dabkowska, K. C. Rule, K. Fritsch, K. Habicht, M. Ramazanoglu","submitted_at":"2015-11-08T13:30:56Z","abstract_excerpt":"The application of a magnetic field transverse to the easy axis, Ising direction in the quasi-two-dimensional Kagome staircase magnet, Co3V2O8, induces three quantum phase transitions at low temperatures, ultimately producing a novel high field polarized state, with two distinct sublattices. New time-of-flight neutron scattering techniques, accompanied by large angular access, high magnetic field infrastructure allow the mapping of a sequence of ferromagnetic and incommensurate phases and their accompanying spin excitations. At least one of the transitions to incommensurate phases at \\mu 0Hc1~"},"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":"1511.02483","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-11-08T13:30:56Z","cross_cats_sorted":[],"title_canon_sha256":"8cedc1dd161939defb9e2c19e90474b4e640425bbdd42b924d51c0e8b1eeea56","abstract_canon_sha256":"21b57d897fbdac21d0f14d62c73ff5f7e2c49d7e9680ced79754990642c67075"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:27:30.161514Z","signature_b64":"+/JkiBbfVwms/qS18VBe7iLVO8wPmZBeltk6RkWs0bKt7eqkC4qdvx4LRFoSqzTPRwpPlIeTtKFLUFKtVhp8DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c55e60b61083cf5b5dec7e4753f47ef0188407eaaa647498c9b0ce7e723b3c8","last_reissued_at":"2026-05-18T01:27:30.160526Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:27:30.160526Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum phase transitions and decoupling of magnetic sublattices in the quasi-two-dimensional Ising magnet Co3V2O8 in a transverse magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. D. Gaulin, G. Ehlers, H. A. Dabkowska, K. C. Rule, K. Fritsch, K. Habicht, M. Ramazanoglu","submitted_at":"2015-11-08T13:30:56Z","abstract_excerpt":"The application of a magnetic field transverse to the easy axis, Ising direction in the quasi-two-dimensional Kagome staircase magnet, Co3V2O8, induces three quantum phase transitions at low temperatures, ultimately producing a novel high field polarized state, with two distinct sublattices. New time-of-flight neutron scattering techniques, accompanied by large angular access, high magnetic field infrastructure allow the mapping of a sequence of ferromagnetic and incommensurate phases and their accompanying spin excitations. At least one of the transitions to incommensurate phases at \\mu 0Hc1~"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.02483","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":"1511.02483","created_at":"2026-05-18T01:27:30.160687+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.02483v1","created_at":"2026-05-18T01:27:30.160687+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.02483","created_at":"2026-05-18T01:27:30.160687+00:00"},{"alias_kind":"pith_short_12","alias_value":"DRK6MC3BBA6P","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"DRK6MC3BBA6PLNO6","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"DRK6MC3B","created_at":"2026-05-18T12:29:17.054201+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/DRK6MC3BBA6PLNO6Y7SHKP2H54","json":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54.json","graph_json":"https://pith.science/api/pith-number/DRK6MC3BBA6PLNO6Y7SHKP2H54/graph.json","events_json":"https://pith.science/api/pith-number/DRK6MC3BBA6PLNO6Y7SHKP2H54/events.json","paper":"https://pith.science/paper/DRK6MC3B"},"agent_actions":{"view_html":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54","download_json":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54.json","view_paper":"https://pith.science/paper/DRK6MC3B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.02483&json=true","fetch_graph":"https://pith.science/api/pith-number/DRK6MC3BBA6PLNO6Y7SHKP2H54/graph.json","fetch_events":"https://pith.science/api/pith-number/DRK6MC3BBA6PLNO6Y7SHKP2H54/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54/action/storage_attestation","attest_author":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54/action/author_attestation","sign_citation":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54/action/citation_signature","submit_replication":"https://pith.science/pith/DRK6MC3BBA6PLNO6Y7SHKP2H54/action/replication_record"}},"created_at":"2026-05-18T01:27:30.160687+00:00","updated_at":"2026-05-18T01:27:30.160687+00:00"}