{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:VWHIQA7B4X4FNJL6KSDDYO435L","short_pith_number":"pith:VWHIQA7B","schema_version":"1.0","canonical_sha256":"ad8e8803e1e5f856a57e54863c3b9beacb271391fd17ff83472e6a6236026dbd","source":{"kind":"arxiv","id":"2506.05085","version":1},"attestation_state":"computed","paper":{"title":"Collective excitation spectra of dipolar bosonic fractional quantum Hall states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Moumita Indra, Pankaj Kumar Mishra","submitted_at":"2025-06-05T14:32:28Z","abstract_excerpt":"We numerically investigate the collective excitation of spin-conserving and spin-reversed configuration of rotating diluted ultra-cold dipolar Bose gas. Rotating trapped Bose gas produces a fictitious magnetic field perpendicular to the trapping harmonic potential, which exhibits strongly correlated fractional quantum Hall states. We consider the long-range dipole-dipole interaction and compute the low lying excitations spectrum for the three fractions of the first Jain series $\\nu = 1/2, 1/4, 1/6$. We find that for both the spin-conserving and spin-reversed excitation the gap between the fund"},"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":"2506.05085","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2025-06-05T14:32:28Z","cross_cats_sorted":[],"title_canon_sha256":"a37130d494ff223c3d8fb7a99d1bbb681ac2e1adfc2ab200062a3b803c5f3665","abstract_canon_sha256":"a301c0e6072ac7847792b64ecf1b46c288117eefeb98cd715bd423396df9ef15"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:16:41.997622Z","signature_b64":"oRTXVC+ZnFQl92oXC7lIArcFDOmCbdLyo98QK4fXEBQVU+iJ5EkjmW3246yq6kaLzwwPZ3YGDVQLCPUcw7xLDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad8e8803e1e5f856a57e54863c3b9beacb271391fd17ff83472e6a6236026dbd","last_reissued_at":"2026-07-05T11:16:41.997068Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:16:41.997068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collective excitation spectra of dipolar bosonic fractional quantum Hall states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Moumita Indra, Pankaj Kumar Mishra","submitted_at":"2025-06-05T14:32:28Z","abstract_excerpt":"We numerically investigate the collective excitation of spin-conserving and spin-reversed configuration of rotating diluted ultra-cold dipolar Bose gas. Rotating trapped Bose gas produces a fictitious magnetic field perpendicular to the trapping harmonic potential, which exhibits strongly correlated fractional quantum Hall states. We consider the long-range dipole-dipole interaction and compute the low lying excitations spectrum for the three fractions of the first Jain series $\\nu = 1/2, 1/4, 1/6$. We find that for both the spin-conserving and spin-reversed excitation the gap between the fund"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.05085","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/2506.05085/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":"2506.05085","created_at":"2026-07-05T11:16:41.997127+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.05085v1","created_at":"2026-07-05T11:16:41.997127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.05085","created_at":"2026-07-05T11:16:41.997127+00:00"},{"alias_kind":"pith_short_12","alias_value":"VWHIQA7B4X4F","created_at":"2026-07-05T11:16:41.997127+00:00"},{"alias_kind":"pith_short_16","alias_value":"VWHIQA7B4X4FNJL6","created_at":"2026-07-05T11:16:41.997127+00:00"},{"alias_kind":"pith_short_8","alias_value":"VWHIQA7B","created_at":"2026-07-05T11:16:41.997127+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/VWHIQA7B4X4FNJL6KSDDYO435L","json":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L.json","graph_json":"https://pith.science/api/pith-number/VWHIQA7B4X4FNJL6KSDDYO435L/graph.json","events_json":"https://pith.science/api/pith-number/VWHIQA7B4X4FNJL6KSDDYO435L/events.json","paper":"https://pith.science/paper/VWHIQA7B"},"agent_actions":{"view_html":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L","download_json":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L.json","view_paper":"https://pith.science/paper/VWHIQA7B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.05085&json=true","fetch_graph":"https://pith.science/api/pith-number/VWHIQA7B4X4FNJL6KSDDYO435L/graph.json","fetch_events":"https://pith.science/api/pith-number/VWHIQA7B4X4FNJL6KSDDYO435L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L/action/storage_attestation","attest_author":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L/action/author_attestation","sign_citation":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L/action/citation_signature","submit_replication":"https://pith.science/pith/VWHIQA7B4X4FNJL6KSDDYO435L/action/replication_record"}},"created_at":"2026-07-05T11:16:41.997127+00:00","updated_at":"2026-07-05T11:16:41.997127+00:00"}