{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:TYWQRWRWOD5BRBJ4Q6PNS3ZBPV","short_pith_number":"pith:TYWQRWRW","schema_version":"1.0","canonical_sha256":"9e2d08da3670fa18853c879ed96f217d622f748c8057f6be612f8eeca3ce893f","source":{"kind":"arxiv","id":"2412.19285","version":1},"attestation_state":"computed","paper":{"title":"Thermal amplification and melting of phases in spin-orbit-coupled spin-1 Bose-Einstein condensates","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Arko Roy, Rajat, Ritu, Sandeep Gautam","submitted_at":"2024-12-26T17:03:05Z","abstract_excerpt":"We implement Hartree-Fock-Bogoliubov theory with Popov approximation for a homogeneous Raman-induced spin-orbit-coupled spin-1 Bose-Einstein condensate and investigate the effects of finite temperature ($T$) on the ground-state phase diagram. We calculate the roton gap as a function of Raman coupling ($\\Omega$) or quadratic Zeeman field strength ($\\epsilon$) to extract the critical points separating the supersolid stripe phase from the plane wave or zero-momentum phase at finite temperatures. We present a few representative finite-temperature phase diagrams for the system in the $T-\\Omega$ and"},"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":"2412.19285","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2024-12-26T17:03:05Z","cross_cats_sorted":[],"title_canon_sha256":"867bd02d029279a038e7b747e7624f236ee955b187abb07eb5df89b81b10ff81","abstract_canon_sha256":"984910989549d889e138d4a1fe8052677a04bc0b65a89c9e090b926afb8bcf70"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:54:33.341786Z","signature_b64":"i7xUkb9jnE0DAidc8vYBQXrntjfGE+m1QO/Ynw0EKEDozduMdGSSi+K3kvu54Yb+y+MyOx0fbJzxfLOyyChoBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e2d08da3670fa18853c879ed96f217d622f748c8057f6be612f8eeca3ce893f","last_reissued_at":"2026-07-05T09:54:33.341396Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:54:33.341396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal amplification and melting of phases in spin-orbit-coupled spin-1 Bose-Einstein condensates","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Arko Roy, Rajat, Ritu, Sandeep Gautam","submitted_at":"2024-12-26T17:03:05Z","abstract_excerpt":"We implement Hartree-Fock-Bogoliubov theory with Popov approximation for a homogeneous Raman-induced spin-orbit-coupled spin-1 Bose-Einstein condensate and investigate the effects of finite temperature ($T$) on the ground-state phase diagram. We calculate the roton gap as a function of Raman coupling ($\\Omega$) or quadratic Zeeman field strength ($\\epsilon$) to extract the critical points separating the supersolid stripe phase from the plane wave or zero-momentum phase at finite temperatures. We present a few representative finite-temperature phase diagrams for the system in the $T-\\Omega$ and"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.19285","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/2412.19285/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":"2412.19285","created_at":"2026-07-05T09:54:33.341452+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.19285v1","created_at":"2026-07-05T09:54:33.341452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.19285","created_at":"2026-07-05T09:54:33.341452+00:00"},{"alias_kind":"pith_short_12","alias_value":"TYWQRWRWOD5B","created_at":"2026-07-05T09:54:33.341452+00:00"},{"alias_kind":"pith_short_16","alias_value":"TYWQRWRWOD5BRBJ4","created_at":"2026-07-05T09:54:33.341452+00:00"},{"alias_kind":"pith_short_8","alias_value":"TYWQRWRW","created_at":"2026-07-05T09:54:33.341452+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/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV","json":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV.json","graph_json":"https://pith.science/api/pith-number/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/graph.json","events_json":"https://pith.science/api/pith-number/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/events.json","paper":"https://pith.science/paper/TYWQRWRW"},"agent_actions":{"view_html":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV","download_json":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV.json","view_paper":"https://pith.science/paper/TYWQRWRW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.19285&json=true","fetch_graph":"https://pith.science/api/pith-number/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/graph.json","fetch_events":"https://pith.science/api/pith-number/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/action/storage_attestation","attest_author":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/action/author_attestation","sign_citation":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/action/citation_signature","submit_replication":"https://pith.science/pith/TYWQRWRWOD5BRBJ4Q6PNS3ZBPV/action/replication_record"}},"created_at":"2026-07-05T09:54:33.341452+00:00","updated_at":"2026-07-05T09:54:33.341452+00:00"}