{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HAR35UONEJDXXJV4TCYLDGXS4I","short_pith_number":"pith:HAR35UON","schema_version":"1.0","canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","source":{"kind":"arxiv","id":"1510.04757","version":2},"attestation_state":"computed","paper":{"title":"Analysis of two and three dipolar bosons in a spherical harmonic trap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. M. Martin, C. J. Bradly, H. M. Quiney","submitted_at":"2015-10-16T01:29:57Z","abstract_excerpt":"As dipolar gases become more readily accessible in experiment there is a need to develop a comprehensive theoretical framework of the few-body physics of these systems. Here, we extend the coupled-pair approach developed for the unitary two-component Fermi gas to a few-body system of dipolar bosons in a spherical harmonic trap. The long range and anisotropy of the dipole-dipole interaction is handled by a flexible and efficient correlated gaussian basis with stochastically variational optimisation. We calculate the eigenenergy spectrum and structural properties of two and three trapped bosonic"},"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":"1510.04757","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-10-16T01:29:57Z","cross_cats_sorted":[],"title_canon_sha256":"b3bd24a621be91df5cbeec7a4f5686abeefcf91c1f06cdbe27a951f3856ced97","abstract_canon_sha256":"39e8b1f9c6d0f7bf592fd51cd1e72e38d2a2d405dc7560c7ff447ad4b13dc3c3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:42.321079Z","signature_b64":"yl2NQDSzd+ID/0k8LvX2/ytRHzyEX9EX6HTpfcZE88GtBq39m1BKDjLsi/3MDos2p6Z6rTe6Ohp37f13BdIZDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","last_reissued_at":"2026-05-18T01:20:42.320636Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:42.320636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of two and three dipolar bosons in a spherical harmonic trap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"A. M. Martin, C. J. Bradly, H. M. Quiney","submitted_at":"2015-10-16T01:29:57Z","abstract_excerpt":"As dipolar gases become more readily accessible in experiment there is a need to develop a comprehensive theoretical framework of the few-body physics of these systems. Here, we extend the coupled-pair approach developed for the unitary two-component Fermi gas to a few-body system of dipolar bosons in a spherical harmonic trap. The long range and anisotropy of the dipole-dipole interaction is handled by a flexible and efficient correlated gaussian basis with stochastically variational optimisation. We calculate the eigenenergy spectrum and structural properties of two and three trapped bosonic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.04757","kind":"arxiv","version":2},"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":"1510.04757","created_at":"2026-05-18T01:20:42.320713+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.04757v2","created_at":"2026-05-18T01:20:42.320713+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.04757","created_at":"2026-05-18T01:20:42.320713+00:00"},{"alias_kind":"pith_short_12","alias_value":"HAR35UONEJDX","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"HAR35UONEJDXXJV4","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"HAR35UON","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/HAR35UONEJDXXJV4TCYLDGXS4I","json":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I.json","graph_json":"https://pith.science/api/pith-number/HAR35UONEJDXXJV4TCYLDGXS4I/graph.json","events_json":"https://pith.science/api/pith-number/HAR35UONEJDXXJV4TCYLDGXS4I/events.json","paper":"https://pith.science/paper/HAR35UON"},"agent_actions":{"view_html":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I","download_json":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I.json","view_paper":"https://pith.science/paper/HAR35UON","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.04757&json=true","fetch_graph":"https://pith.science/api/pith-number/HAR35UONEJDXXJV4TCYLDGXS4I/graph.json","fetch_events":"https://pith.science/api/pith-number/HAR35UONEJDXXJV4TCYLDGXS4I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/action/storage_attestation","attest_author":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/action/author_attestation","sign_citation":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/action/citation_signature","submit_replication":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/action/replication_record"}},"created_at":"2026-05-18T01:20:42.320713+00:00","updated_at":"2026-05-18T01:20:42.320713+00:00"}