{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:FXMB27BJRH46X27RY2LHLWYP42","short_pith_number":"pith:FXMB27BJ","schema_version":"1.0","canonical_sha256":"2dd81d7c2989f9ebebf1c69675db0fe69331e6ce0a0da28c4ea4745b144d0276","source":{"kind":"arxiv","id":"1503.00300","version":1},"attestation_state":"computed","paper":{"title":"Spinor Condensates on a Cylindrical Surface in Synthetic Gauge Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Biao Huang, Tin-Lun Ho","submitted_at":"2015-03-01T16:39:57Z","abstract_excerpt":"We point out that by modifying the setup of a recent experiment that generates a Dirac string, one can create a quasi 2D spinor Bose condensate on a cylindrical surface with a synthetic magnetic field pointing radially outward from the cylindrical surface. The synthetic magnetic field takes the form of the Landau gauge. It is generated by the Berry's phase of a spin texture, frozen by an external quadrupolar magnetic field. Unlike in the planar case, there are two types of vortices (called A and B) with the same vorticity. The ground state for $5\\le S\\le 9$ consists of a row of alternating AB "},"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":"1503.00300","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-03-01T16:39:57Z","cross_cats_sorted":[],"title_canon_sha256":"7dabe88d94afd346cb604806bcf596fd3f1292ecdc09bcb77ddf547857da2d42","abstract_canon_sha256":"e9b1c0b92b54263cf39de6c183e354240163ffec983b53b6af881088254e4697"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:25.138154Z","signature_b64":"sHcxSXNkgVPny3IPEffqB23JiMhN/gQAyGxyYcIRoZ/zJzvo0TTK2fzwcBWrZFUaLzrwlddC943WHTvZvC3ZCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2dd81d7c2989f9ebebf1c69675db0fe69331e6ce0a0da28c4ea4745b144d0276","last_reissued_at":"2026-05-18T01:30:25.137278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:25.137278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spinor Condensates on a Cylindrical Surface in Synthetic Gauge Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Biao Huang, Tin-Lun Ho","submitted_at":"2015-03-01T16:39:57Z","abstract_excerpt":"We point out that by modifying the setup of a recent experiment that generates a Dirac string, one can create a quasi 2D spinor Bose condensate on a cylindrical surface with a synthetic magnetic field pointing radially outward from the cylindrical surface. The synthetic magnetic field takes the form of the Landau gauge. It is generated by the Berry's phase of a spin texture, frozen by an external quadrupolar magnetic field. Unlike in the planar case, there are two types of vortices (called A and B) with the same vorticity. The ground state for $5\\le S\\le 9$ consists of a row of alternating AB "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.00300","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":"1503.00300","created_at":"2026-05-18T01:30:25.137434+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.00300v1","created_at":"2026-05-18T01:30:25.137434+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.00300","created_at":"2026-05-18T01:30:25.137434+00:00"},{"alias_kind":"pith_short_12","alias_value":"FXMB27BJRH46","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"FXMB27BJRH46X27R","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"FXMB27BJ","created_at":"2026-05-18T12:29:22.688609+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/FXMB27BJRH46X27RY2LHLWYP42","json":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42.json","graph_json":"https://pith.science/api/pith-number/FXMB27BJRH46X27RY2LHLWYP42/graph.json","events_json":"https://pith.science/api/pith-number/FXMB27BJRH46X27RY2LHLWYP42/events.json","paper":"https://pith.science/paper/FXMB27BJ"},"agent_actions":{"view_html":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42","download_json":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42.json","view_paper":"https://pith.science/paper/FXMB27BJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.00300&json=true","fetch_graph":"https://pith.science/api/pith-number/FXMB27BJRH46X27RY2LHLWYP42/graph.json","fetch_events":"https://pith.science/api/pith-number/FXMB27BJRH46X27RY2LHLWYP42/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42/action/storage_attestation","attest_author":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42/action/author_attestation","sign_citation":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42/action/citation_signature","submit_replication":"https://pith.science/pith/FXMB27BJRH46X27RY2LHLWYP42/action/replication_record"}},"created_at":"2026-05-18T01:30:25.137434+00:00","updated_at":"2026-05-18T01:30:25.137434+00:00"}