{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JTQ3PTXX3WPBCXGZ7DCLLFI4BW","short_pith_number":"pith:JTQ3PTXX","schema_version":"1.0","canonical_sha256":"4ce1b7cef7dd9e115cd9f8c4b5951c0d80e1fa5aa8716946cdd569d1dafd145a","source":{"kind":"arxiv","id":"1607.03956","version":1},"attestation_state":"computed","paper":{"title":"Morphing of 2D Hole Systems at $\\nu=3/2$ in Parallel Magnetic Fields: Compressible, Stripe, and Fractional Quantum Hall Phases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"K.W. Baldwin, K.W. West, L.N. Pfeiffer, M. A. Mueed, Md. Shafayat Hossain, M. Shayegan, S. Hasdermir, Yang Liu","submitted_at":"2016-07-13T23:21:43Z","abstract_excerpt":"A transport study of two-dimensional (2D) holes confined to wide GaAs quantum wells provides a glimpse of a subtle competition between different many-body phases at Landau level filling $\\nu=3/2$ in tilted magnetic fields. At large tilt angles ($\\theta$), an anisotropic, stripe (or nematic) phase replaces the isotropic compressible Fermi sea at $\\nu=3/2$ if the quantum well has a symmetric charge distribution. When the charge distribution is made asymmetric, instead of the stripe phase, an even-denominator fractional quantum state appears at $\\nu=3/2$ in a range of large $\\theta$, and reverts "},"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":"1607.03956","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-07-13T23:21:43Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"3f138d86c509ca0dafbcf575d04f33ecf1362c29da028b15493deaded3d876f5","abstract_canon_sha256":"958960c88d05e5d06606a800cad386be7a43d746f452a9e1113f7aac48d3307a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:00:05.658711Z","signature_b64":"o7dPmGVNFcRvzt/jcxvj97a9lClGtDIRg9nKLeWJZ+l+dAmjjr1PemMJln5dPqEKjJ2bVZ7BhLWyBjBUYOpcAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ce1b7cef7dd9e115cd9f8c4b5951c0d80e1fa5aa8716946cdd569d1dafd145a","last_reissued_at":"2026-05-18T01:00:05.658219Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:00:05.658219Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Morphing of 2D Hole Systems at $\\nu=3/2$ in Parallel Magnetic Fields: Compressible, Stripe, and Fractional Quantum Hall Phases","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"K.W. Baldwin, K.W. West, L.N. Pfeiffer, M. A. Mueed, Md. Shafayat Hossain, M. Shayegan, S. Hasdermir, Yang Liu","submitted_at":"2016-07-13T23:21:43Z","abstract_excerpt":"A transport study of two-dimensional (2D) holes confined to wide GaAs quantum wells provides a glimpse of a subtle competition between different many-body phases at Landau level filling $\\nu=3/2$ in tilted magnetic fields. At large tilt angles ($\\theta$), an anisotropic, stripe (or nematic) phase replaces the isotropic compressible Fermi sea at $\\nu=3/2$ if the quantum well has a symmetric charge distribution. When the charge distribution is made asymmetric, instead of the stripe phase, an even-denominator fractional quantum state appears at $\\nu=3/2$ in a range of large $\\theta$, and reverts "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.03956","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":"1607.03956","created_at":"2026-05-18T01:00:05.658305+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.03956v1","created_at":"2026-05-18T01:00:05.658305+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.03956","created_at":"2026-05-18T01:00:05.658305+00:00"},{"alias_kind":"pith_short_12","alias_value":"JTQ3PTXX3WPB","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JTQ3PTXX3WPBCXGZ","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JTQ3PTXX","created_at":"2026-05-18T12:30:25.849896+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/JTQ3PTXX3WPBCXGZ7DCLLFI4BW","json":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW.json","graph_json":"https://pith.science/api/pith-number/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/graph.json","events_json":"https://pith.science/api/pith-number/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/events.json","paper":"https://pith.science/paper/JTQ3PTXX"},"agent_actions":{"view_html":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW","download_json":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW.json","view_paper":"https://pith.science/paper/JTQ3PTXX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.03956&json=true","fetch_graph":"https://pith.science/api/pith-number/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/graph.json","fetch_events":"https://pith.science/api/pith-number/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/action/storage_attestation","attest_author":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/action/author_attestation","sign_citation":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/action/citation_signature","submit_replication":"https://pith.science/pith/JTQ3PTXX3WPBCXGZ7DCLLFI4BW/action/replication_record"}},"created_at":"2026-05-18T01:00:05.658305+00:00","updated_at":"2026-05-18T01:00:05.658305+00:00"}