{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:LVOQG7C5GK6SW6X7AMAEPUP6L6","short_pith_number":"pith:LVOQG7C5","schema_version":"1.0","canonical_sha256":"5d5d037c5d32bd2b7aff030047d1fe5fa3eef8c91808bba020caaf64abde6ae8","source":{"kind":"arxiv","id":"2103.13930","version":1},"attestation_state":"computed","paper":{"title":"Pattern Formation in Quantum Ferrofluids: from Supersolids to Superglasses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"F. B\\\"ottcher, J. Hertkorn, J.-N. Schmidt, K.S.H. Ng, M. Guo, M. Zwierlein, P. Uerlings, S.D. Graham, T. Langen, T. Pfau","submitted_at":"2021-03-25T15:42:40Z","abstract_excerpt":"Pattern formation is a ubiquitous phenomenon observed in nonlinear and out-of-equilibrium systems. In equilibrium, quantum ferrofluids formed from ultracold atoms were recently shown to spontaneously develop coherent density patterns, manifesting a supersolid. We theoretically investigate the phase diagram of such quantum ferrofluids in oblate trap geometries and find an even wider range of exotic states of matter. Two-dimensional supersolid crystals formed from individual ferrofluid quantum droplets dominate the phase diagram at low densities. For higher densities we find honeycomb and labyri"},"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":"2103.13930","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2021-03-25T15:42:40Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"c89ca35399be5c93e7e3b810fca399ec509942268310b01b5f64035950faa754","abstract_canon_sha256":"aa63f976a0ea94b1c37e5375d490e867f3dce50fd418e3a4f9164945aaa00409"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:04:48.379707Z","signature_b64":"CRXdnUoqUUC4nJDn6WJgIjHwCtc97CBFp3WhztcytEc48E08D38dStsZpObFilqrvszsbUGFwJObICwHbxl6DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d5d037c5d32bd2b7aff030047d1fe5fa3eef8c91808bba020caaf64abde6ae8","last_reissued_at":"2026-07-05T03:04:48.379224Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:04:48.379224Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pattern Formation in Quantum Ferrofluids: from Supersolids to Superglasses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"F. B\\\"ottcher, J. Hertkorn, J.-N. Schmidt, K.S.H. Ng, M. Guo, M. Zwierlein, P. Uerlings, S.D. Graham, T. Langen, T. Pfau","submitted_at":"2021-03-25T15:42:40Z","abstract_excerpt":"Pattern formation is a ubiquitous phenomenon observed in nonlinear and out-of-equilibrium systems. In equilibrium, quantum ferrofluids formed from ultracold atoms were recently shown to spontaneously develop coherent density patterns, manifesting a supersolid. We theoretically investigate the phase diagram of such quantum ferrofluids in oblate trap geometries and find an even wider range of exotic states of matter. Two-dimensional supersolid crystals formed from individual ferrofluid quantum droplets dominate the phase diagram at low densities. For higher densities we find honeycomb and labyri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.13930","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/2103.13930/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":"2103.13930","created_at":"2026-07-05T03:04:48.379279+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.13930v1","created_at":"2026-07-05T03:04:48.379279+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.13930","created_at":"2026-07-05T03:04:48.379279+00:00"},{"alias_kind":"pith_short_12","alias_value":"LVOQG7C5GK6S","created_at":"2026-07-05T03:04:48.379279+00:00"},{"alias_kind":"pith_short_16","alias_value":"LVOQG7C5GK6SW6X7","created_at":"2026-07-05T03:04:48.379279+00:00"},{"alias_kind":"pith_short_8","alias_value":"LVOQG7C5","created_at":"2026-07-05T03:04:48.379279+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/LVOQG7C5GK6SW6X7AMAEPUP6L6","json":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6.json","graph_json":"https://pith.science/api/pith-number/LVOQG7C5GK6SW6X7AMAEPUP6L6/graph.json","events_json":"https://pith.science/api/pith-number/LVOQG7C5GK6SW6X7AMAEPUP6L6/events.json","paper":"https://pith.science/paper/LVOQG7C5"},"agent_actions":{"view_html":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6","download_json":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6.json","view_paper":"https://pith.science/paper/LVOQG7C5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.13930&json=true","fetch_graph":"https://pith.science/api/pith-number/LVOQG7C5GK6SW6X7AMAEPUP6L6/graph.json","fetch_events":"https://pith.science/api/pith-number/LVOQG7C5GK6SW6X7AMAEPUP6L6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6/action/storage_attestation","attest_author":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6/action/author_attestation","sign_citation":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6/action/citation_signature","submit_replication":"https://pith.science/pith/LVOQG7C5GK6SW6X7AMAEPUP6L6/action/replication_record"}},"created_at":"2026-07-05T03:04:48.379279+00:00","updated_at":"2026-07-05T03:04:48.379279+00:00"}