{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:XYCF72OIZAATEKITC7NBLGGLYN","short_pith_number":"pith:XYCF72OI","schema_version":"1.0","canonical_sha256":"be045fe9c8c80132291317da1598cbc37b63468b2bb869dff4d9896062804e2f","source":{"kind":"arxiv","id":"2606.24939","version":1},"attestation_state":"computed","paper":{"title":"Bright-state source cancellation in dissipative shortcut Raman atom optics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.atom-ph","physics.optics"],"primary_cat":"quant-ph","authors_text":"Asad Ali, H. Kuniyil, M. I. Hussain, M. T. Rahim, Saeed Haddadi, Saif Al-Kuwari","submitted_at":"2026-06-22T19:21:15Z","abstract_excerpt":"Spontaneous Raman scattering limits shortcut-assisted atom optics, but its microscopic origin is obscured once the lossy excited state is adiabatically eliminated. We organize the problem around a single quantity: in the instantaneous dark-bright basis the lower-manifold optical source is carried entirely by the bright-state amplitude, $S=\\Omega b$, so that primary spontaneous scattering reduces to the compact functional. This recovers the known dissipative-STIRAP loss in transparent form and makes the action of a shortcut explicit: ideal counterdiabatic STIRSAP cancels the bright-state \\emph{"},"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":"2606.24939","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-06-22T19:21:15Z","cross_cats_sorted":["physics.atom-ph","physics.optics"],"title_canon_sha256":"5ca6495a1164a80832ea580e52d254c803617369fb16bcdaa45ec27cfeffd4c8","abstract_canon_sha256":"a30425841847741f93c43af2e4a62e463b9b6dc4e712b16b1c96a106c53d194a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-25T00:17:46.431591Z","signature_b64":"PnIUe/tk38wUOpomP2NfChZ/mU7hRMBkL/HGobWbh0wCD7Vl40ZgtWuEdbvLx/vyXRHWAMjWLdu2tdFOezziBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be045fe9c8c80132291317da1598cbc37b63468b2bb869dff4d9896062804e2f","last_reissued_at":"2026-06-25T00:17:46.431234Z","signature_status":"signed_v1","first_computed_at":"2026-06-25T00:17:46.431234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bright-state source cancellation in dissipative shortcut Raman atom optics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.atom-ph","physics.optics"],"primary_cat":"quant-ph","authors_text":"Asad Ali, H. Kuniyil, M. I. Hussain, M. T. Rahim, Saeed Haddadi, Saif Al-Kuwari","submitted_at":"2026-06-22T19:21:15Z","abstract_excerpt":"Spontaneous Raman scattering limits shortcut-assisted atom optics, but its microscopic origin is obscured once the lossy excited state is adiabatically eliminated. We organize the problem around a single quantity: in the instantaneous dark-bright basis the lower-manifold optical source is carried entirely by the bright-state amplitude, $S=\\Omega b$, so that primary spontaneous scattering reduces to the compact functional. This recovers the known dissipative-STIRAP loss in transparent form and makes the action of a shortcut explicit: ideal counterdiabatic STIRSAP cancels the bright-state \\emph{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.24939","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/2606.24939/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":"2606.24939","created_at":"2026-06-25T00:17:46.431295+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.24939v1","created_at":"2026-06-25T00:17:46.431295+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.24939","created_at":"2026-06-25T00:17:46.431295+00:00"},{"alias_kind":"pith_short_12","alias_value":"XYCF72OIZAAT","created_at":"2026-06-25T00:17:46.431295+00:00"},{"alias_kind":"pith_short_16","alias_value":"XYCF72OIZAATEKIT","created_at":"2026-06-25T00:17:46.431295+00:00"},{"alias_kind":"pith_short_8","alias_value":"XYCF72OI","created_at":"2026-06-25T00:17:46.431295+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/XYCF72OIZAATEKITC7NBLGGLYN","json":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN.json","graph_json":"https://pith.science/api/pith-number/XYCF72OIZAATEKITC7NBLGGLYN/graph.json","events_json":"https://pith.science/api/pith-number/XYCF72OIZAATEKITC7NBLGGLYN/events.json","paper":"https://pith.science/paper/XYCF72OI"},"agent_actions":{"view_html":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN","download_json":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN.json","view_paper":"https://pith.science/paper/XYCF72OI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.24939&json=true","fetch_graph":"https://pith.science/api/pith-number/XYCF72OIZAATEKITC7NBLGGLYN/graph.json","fetch_events":"https://pith.science/api/pith-number/XYCF72OIZAATEKITC7NBLGGLYN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN/action/storage_attestation","attest_author":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN/action/author_attestation","sign_citation":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN/action/citation_signature","submit_replication":"https://pith.science/pith/XYCF72OIZAATEKITC7NBLGGLYN/action/replication_record"}},"created_at":"2026-06-25T00:17:46.431295+00:00","updated_at":"2026-06-25T00:17:46.431295+00:00"}