{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:HAR35UONEJDXXJV4TCYLDGXS4I","short_pith_number":"pith:HAR35UON","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"},"canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","source":{"kind":"arxiv","id":"1510.04757","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.04757","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"arxiv_version","alias_value":"1510.04757v2","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.04757","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"pith_short_12","alias_value":"HAR35UONEJDX","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"HAR35UONEJDXXJV4","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"HAR35UON","created_at":"2026-05-18T12:29:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:HAR35UONEJDXXJV4TCYLDGXS4I","target":"record","payload":{"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"},"canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","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"},"source_kind":"arxiv","source_id":"1510.04757","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:20:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qCqu/q9wqJ+f+iYoD46sgdZmEUAHryIywycBJohYOh2hXw3JuVzwlsnk3L+Zgd77+4v9CZ8Iw8OsU4xLZ+avDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:38:32.078489Z"},"content_sha256":"890aa00de5550972175ec7ab1b3beac2a3d823968bce87a40e6bedfdb97a6ee8","schema_version":"1.0","event_id":"sha256:890aa00de5550972175ec7ab1b3beac2a3d823968bce87a40e6bedfdb97a6ee8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:HAR35UONEJDXXJV4TCYLDGXS4I","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:20:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Aa1GCPMbYFMsSd8VXulFaWOkkU1Mn9H/MZmO439EeBxs9L2yEwC7PUrs9Wog9BbPr2cXC2bgqhX9i+HGHZAtAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:38:32.079209Z"},"content_sha256":"e6830dc8db09d20637c6f8bd3d7761cc792155f08ac43e512403befc9e2a3d48","schema_version":"1.0","event_id":"sha256:e6830dc8db09d20637c6f8bd3d7761cc792155f08ac43e512403befc9e2a3d48"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/bundle.json","state_url":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HAR35UONEJDXXJV4TCYLDGXS4I/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-27T21:38:32Z","links":{"resolver":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I","bundle":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/bundle.json","state":"https://pith.science/pith/HAR35UONEJDXXJV4TCYLDGXS4I/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HAR35UONEJDXXJV4TCYLDGXS4I/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:HAR35UONEJDXXJV4TCYLDGXS4I","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"39e8b1f9c6d0f7bf592fd51cd1e72e38d2a2d405dc7560c7ff447ad4b13dc3c3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-10-16T01:29:57Z","title_canon_sha256":"b3bd24a621be91df5cbeec7a4f5686abeefcf91c1f06cdbe27a951f3856ced97"},"schema_version":"1.0","source":{"id":"1510.04757","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.04757","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"arxiv_version","alias_value":"1510.04757v2","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.04757","created_at":"2026-05-18T01:20:42Z"},{"alias_kind":"pith_short_12","alias_value":"HAR35UONEJDX","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"HAR35UONEJDXXJV4","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"HAR35UON","created_at":"2026-05-18T12:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:e6830dc8db09d20637c6f8bd3d7761cc792155f08ac43e512403befc9e2a3d48","target":"graph","created_at":"2026-05-18T01:20:42Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"A. M. Martin, C. J. Bradly, H. M. Quiney","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-10-16T01:29:57Z","title":"Analysis of two and three dipolar bosons in a spherical harmonic trap"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.04757","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:890aa00de5550972175ec7ab1b3beac2a3d823968bce87a40e6bedfdb97a6ee8","target":"record","created_at":"2026-05-18T01:20:42Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"39e8b1f9c6d0f7bf592fd51cd1e72e38d2a2d405dc7560c7ff447ad4b13dc3c3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-10-16T01:29:57Z","title_canon_sha256":"b3bd24a621be91df5cbeec7a4f5686abeefcf91c1f06cdbe27a951f3856ced97"},"schema_version":"1.0","source":{"id":"1510.04757","kind":"arxiv","version":2}},"canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3823bed1cd22477ba6bc98b0b19af2e20e2632da6b0e415c38083459533ba61e","first_computed_at":"2026-05-18T01:20:42.320636Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:20:42.320636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yl2NQDSzd+ID/0k8LvX2/ytRHzyEX9EX6HTpfcZE88GtBq39m1BKDjLsi/3MDos2p6Z6rTe6Ohp37f13BdIZDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:20:42.321079Z","signed_message":"canonical_sha256_bytes"},"source_id":"1510.04757","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:890aa00de5550972175ec7ab1b3beac2a3d823968bce87a40e6bedfdb97a6ee8","sha256:e6830dc8db09d20637c6f8bd3d7761cc792155f08ac43e512403befc9e2a3d48"],"state_sha256":"11332aa1a19577271aa5494b7b2232063f1024bc09456fc8cae183904c05ff69"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1xMV9S2ELiytUsUMwCKvmjZQ3dvoaj6+9zkDQmC9v+QLDW+n3OnY5TEngGvvoqePIzvMTnFtY/oe8ALMzbwmBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:38:32.083037Z","bundle_sha256":"f552c981f7815be4fd5e796accb631357272cb890e5ebed2f32b557b66797701"}}