{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:P4ZHOV772SNFF3X723DYXCZAU2","short_pith_number":"pith:P4ZHOV77","schema_version":"1.0","canonical_sha256":"7f327757ffd49a52eeffd6c78b8b20a696f6adce1b35fa279aaba7abf6e9b9d5","source":{"kind":"arxiv","id":"1103.5697","version":1},"attestation_state":"computed","paper":{"title":"Initial value representation for the SU(n) semiclassical propagator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Marcus A. M. de Aguiar, Thiago F. Viscondi","submitted_at":"2011-03-29T16:07:52Z","abstract_excerpt":"The semiclassical propagator in the representation of SU(n) coherent states is characterized by isolated classical trajectories subjected to boundary conditions in a doubled phase space. In this paper we recast this expression in terms of an integral over a set of initial-valued trajectories. These trajectories are monitored by a filter that collects only the appropriate contributions to the semiclassical approximation. This framework is suitable for the study of bosonic dynamics in n modes with fixed total number of particles. We exemplify the method for a Bose-Einstein condensate trapped in "},"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":"1103.5697","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-03-29T16:07:52Z","cross_cats_sorted":[],"title_canon_sha256":"b74b98b5dc7a76f753dd3ab0657dbfee765a575496cd53807f5c7914d336b031","abstract_canon_sha256":"883af0010762509b66c247fceafbd96fc3c94685072d072ace418b098339594d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:18:54.397123Z","signature_b64":"RmzC+2e8nek1R5pjHNIxrpR8uinMo8W0vLsuMP6+u1D2saxMzG/Em5mn8GulkpSQMTpL7rAO1Zkq+jxWRv59BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f327757ffd49a52eeffd6c78b8b20a696f6adce1b35fa279aaba7abf6e9b9d5","last_reissued_at":"2026-05-18T04:18:54.396717Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:18:54.396717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Initial value representation for the SU(n) semiclassical propagator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Marcus A. M. de Aguiar, Thiago F. Viscondi","submitted_at":"2011-03-29T16:07:52Z","abstract_excerpt":"The semiclassical propagator in the representation of SU(n) coherent states is characterized by isolated classical trajectories subjected to boundary conditions in a doubled phase space. In this paper we recast this expression in terms of an integral over a set of initial-valued trajectories. These trajectories are monitored by a filter that collects only the appropriate contributions to the semiclassical approximation. This framework is suitable for the study of bosonic dynamics in n modes with fixed total number of particles. We exemplify the method for a Bose-Einstein condensate trapped in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.5697","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":""},"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":"1103.5697","created_at":"2026-05-18T04:18:54.396779+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.5697v1","created_at":"2026-05-18T04:18:54.396779+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.5697","created_at":"2026-05-18T04:18:54.396779+00:00"},{"alias_kind":"pith_short_12","alias_value":"P4ZHOV772SNF","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"P4ZHOV772SNFF3X7","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"P4ZHOV77","created_at":"2026-05-18T12:26:39.201973+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/P4ZHOV772SNFF3X723DYXCZAU2","json":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2.json","graph_json":"https://pith.science/api/pith-number/P4ZHOV772SNFF3X723DYXCZAU2/graph.json","events_json":"https://pith.science/api/pith-number/P4ZHOV772SNFF3X723DYXCZAU2/events.json","paper":"https://pith.science/paper/P4ZHOV77"},"agent_actions":{"view_html":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2","download_json":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2.json","view_paper":"https://pith.science/paper/P4ZHOV77","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.5697&json=true","fetch_graph":"https://pith.science/api/pith-number/P4ZHOV772SNFF3X723DYXCZAU2/graph.json","fetch_events":"https://pith.science/api/pith-number/P4ZHOV772SNFF3X723DYXCZAU2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2/action/storage_attestation","attest_author":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2/action/author_attestation","sign_citation":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2/action/citation_signature","submit_replication":"https://pith.science/pith/P4ZHOV772SNFF3X723DYXCZAU2/action/replication_record"}},"created_at":"2026-05-18T04:18:54.396779+00:00","updated_at":"2026-05-18T04:18:54.396779+00:00"}