{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:SPU6PZKHGQN4FD2RRZZRYMHUSJ","short_pith_number":"pith:SPU6PZKH","schema_version":"1.0","canonical_sha256":"93e9e7e547341bc28f518e731c30f4924475fe5f0aff975440e777994de5f3af","source":{"kind":"arxiv","id":"2507.22354","version":1},"attestation_state":"computed","paper":{"title":"Universal Magnetic Phases in Twisted Bilayer MoTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andrea F. Young, Canxun Zhang, Chaowei Hu, Christiano Wang Beach, Di Xiao, Eric Anderson, Evgeny Redekop, Heonjoon Park, Jiun-Haw Chu, Kenji Watanabe, Liang Fu, Takashi Taniguchi, Ting Cao, Weijie Li, Will Holtzmann, Xiaodong Xu, Xiaowei Zhang, Xiaoyu Liu","submitted_at":"2025-07-30T03:35:54Z","abstract_excerpt":"Twisted bilayer MoTe$_2$ (tMoTe$_2$) has emerged as a robust platform for exploring correlated topological phases, notably supporting fractional Chern insulator (FCI) states at zero magnetic field across a wide range of twist angles. The evolution of magnetism and topology with twist angle remains an open question. Here, we systematically map the magnetic phase diagram of tMoTe$_2$ using local optical spectroscopy and scanning nanoSQUID-on-tip (nSOT) magnetometry. We identify spontaneous ferromagnetism at moir\\'e filling factors $\\nu = -1$ and $-3$ over a twist angle range from 2.1$^\\circ$ to "},"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":"2507.22354","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-07-30T03:35:54Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"14ddbe3120ba5e4040a94924c1a46177213011365f02d411fbbd0e307d54b06b","abstract_canon_sha256":"f2ac5b47e3bac1ca3a172c3c55a4501d6438004c58a31403f32732e8492620eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:45:39.910602Z","signature_b64":"c8K/qk8o2PyxWLAClAsP2ZPUVJrGmd4QPAKvR2624R4b0+wArEoIW5sw+SZxgRKdHbvmAf2CHhddO3SWngMqBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93e9e7e547341bc28f518e731c30f4924475fe5f0aff975440e777994de5f3af","last_reissued_at":"2026-07-05T11:45:39.910088Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:45:39.910088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal Magnetic Phases in Twisted Bilayer MoTe$_2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andrea F. Young, Canxun Zhang, Chaowei Hu, Christiano Wang Beach, Di Xiao, Eric Anderson, Evgeny Redekop, Heonjoon Park, Jiun-Haw Chu, Kenji Watanabe, Liang Fu, Takashi Taniguchi, Ting Cao, Weijie Li, Will Holtzmann, Xiaodong Xu, Xiaowei Zhang, Xiaoyu Liu","submitted_at":"2025-07-30T03:35:54Z","abstract_excerpt":"Twisted bilayer MoTe$_2$ (tMoTe$_2$) has emerged as a robust platform for exploring correlated topological phases, notably supporting fractional Chern insulator (FCI) states at zero magnetic field across a wide range of twist angles. The evolution of magnetism and topology with twist angle remains an open question. Here, we systematically map the magnetic phase diagram of tMoTe$_2$ using local optical spectroscopy and scanning nanoSQUID-on-tip (nSOT) magnetometry. We identify spontaneous ferromagnetism at moir\\'e filling factors $\\nu = -1$ and $-3$ over a twist angle range from 2.1$^\\circ$ to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.22354","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2507.22354/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2507.22354","created_at":"2026-07-05T11:45:39.910147+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.22354v1","created_at":"2026-07-05T11:45:39.910147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.22354","created_at":"2026-07-05T11:45:39.910147+00:00"},{"alias_kind":"pith_short_12","alias_value":"SPU6PZKHGQN4","created_at":"2026-07-05T11:45:39.910147+00:00"},{"alias_kind":"pith_short_16","alias_value":"SPU6PZKHGQN4FD2R","created_at":"2026-07-05T11:45:39.910147+00:00"},{"alias_kind":"pith_short_8","alias_value":"SPU6PZKH","created_at":"2026-07-05T11:45:39.910147+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.01727","citing_title":"Orbital Magnetization of Correlated States in Twisted Bilayer Transition Metal Dichalcogenides","ref_index":13,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ","json":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ.json","graph_json":"https://pith.science/api/pith-number/SPU6PZKHGQN4FD2RRZZRYMHUSJ/graph.json","events_json":"https://pith.science/api/pith-number/SPU6PZKHGQN4FD2RRZZRYMHUSJ/events.json","paper":"https://pith.science/paper/SPU6PZKH"},"agent_actions":{"view_html":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ","download_json":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ.json","view_paper":"https://pith.science/paper/SPU6PZKH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.22354&json=true","fetch_graph":"https://pith.science/api/pith-number/SPU6PZKHGQN4FD2RRZZRYMHUSJ/graph.json","fetch_events":"https://pith.science/api/pith-number/SPU6PZKHGQN4FD2RRZZRYMHUSJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ/action/storage_attestation","attest_author":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ/action/author_attestation","sign_citation":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ/action/citation_signature","submit_replication":"https://pith.science/pith/SPU6PZKHGQN4FD2RRZZRYMHUSJ/action/replication_record"}},"created_at":"2026-07-05T11:45:39.910147+00:00","updated_at":"2026-07-05T11:45:39.910147+00:00"}