{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:VNC3RMQT5VFCRR4A6NPCAOSO6L","short_pith_number":"pith:VNC3RMQT","schema_version":"1.0","canonical_sha256":"ab45b8b213ed4a28c780f35e203a4ef2ce35d859c1599d5efae4862286f18222","source":{"kind":"arxiv","id":"2006.00841","version":1},"attestation_state":"computed","paper":{"title":"Quantum polar decomposition algorithm","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Bobak Kiani, David M. Arvidsson-Shukur, Giacomo De Palma, Milad Marvian, Patrick Rebentrost, Samuel Bosch, Seth Lloyd, Zi-Wen Liu","submitted_at":"2020-06-01T10:34:24Z","abstract_excerpt":"The polar decomposition for a matrix $A$ is $A=UB$, where $B$ is a positive Hermitian matrix and $U$ is unitary (or, if $A$ is not square, an isometry). This paper shows that the ability to apply a Hamiltonian $\\pmatrix{ 0 & A^\\dagger \\cr A & 0 \\cr} $ translates into the ability to perform the transformations $e^{-iBt}$ and $U$ in a deterministic fashion. We show how to use the quantum polar decomposition algorithm to solve the quantum Procrustes problem, to perform pretty good measurements, to find the positive Hamiltonian closest to any Hamiltonian, and to perform a Hamiltonian version of th"},"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":"2006.00841","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-06-01T10:34:24Z","cross_cats_sorted":[],"title_canon_sha256":"8218fbf466f3aaf50c4b2965141899035fced257f1ac56dc01d1cac3d9a4ffb2","abstract_canon_sha256":"7dbe2032522d30fcda6ed0b550652434b7b9dad08458d31794a7cf798a949776"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:07:06.075672Z","signature_b64":"pXWNtT4F6OPFyUCoDzb3aoEDS/WNidvFwHjhNOIg1lnVKhr5jWem68nje+hgRVHNvyh5ixoN8JyMlEnEnGFIBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab45b8b213ed4a28c780f35e203a4ef2ce35d859c1599d5efae4862286f18222","last_reissued_at":"2026-07-05T01:07:06.075170Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:07:06.075170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum polar decomposition algorithm","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Bobak Kiani, David M. Arvidsson-Shukur, Giacomo De Palma, Milad Marvian, Patrick Rebentrost, Samuel Bosch, Seth Lloyd, Zi-Wen Liu","submitted_at":"2020-06-01T10:34:24Z","abstract_excerpt":"The polar decomposition for a matrix $A$ is $A=UB$, where $B$ is a positive Hermitian matrix and $U$ is unitary (or, if $A$ is not square, an isometry). This paper shows that the ability to apply a Hamiltonian $\\pmatrix{ 0 & A^\\dagger \\cr A & 0 \\cr} $ translates into the ability to perform the transformations $e^{-iBt}$ and $U$ in a deterministic fashion. We show how to use the quantum polar decomposition algorithm to solve the quantum Procrustes problem, to perform pretty good measurements, to find the positive Hamiltonian closest to any Hamiltonian, and to perform a Hamiltonian version of th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2006.00841","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/2006.00841/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":"2006.00841","created_at":"2026-07-05T01:07:06.075236+00:00"},{"alias_kind":"arxiv_version","alias_value":"2006.00841v1","created_at":"2026-07-05T01:07:06.075236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2006.00841","created_at":"2026-07-05T01:07:06.075236+00:00"},{"alias_kind":"pith_short_12","alias_value":"VNC3RMQT5VFC","created_at":"2026-07-05T01:07:06.075236+00:00"},{"alias_kind":"pith_short_16","alias_value":"VNC3RMQT5VFCRR4A","created_at":"2026-07-05T01:07:06.075236+00:00"},{"alias_kind":"pith_short_8","alias_value":"VNC3RMQT","created_at":"2026-07-05T01:07:06.075236+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.17357","citing_title":"Pulse-optimised circuit elements for scalable and noise-resilient quantum chemistry","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2602.09575","citing_title":"Quantum Simulation of Non-Unitary Dynamics via Amplitude-Phase Separation","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L","json":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L.json","graph_json":"https://pith.science/api/pith-number/VNC3RMQT5VFCRR4A6NPCAOSO6L/graph.json","events_json":"https://pith.science/api/pith-number/VNC3RMQT5VFCRR4A6NPCAOSO6L/events.json","paper":"https://pith.science/paper/VNC3RMQT"},"agent_actions":{"view_html":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L","download_json":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L.json","view_paper":"https://pith.science/paper/VNC3RMQT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2006.00841&json=true","fetch_graph":"https://pith.science/api/pith-number/VNC3RMQT5VFCRR4A6NPCAOSO6L/graph.json","fetch_events":"https://pith.science/api/pith-number/VNC3RMQT5VFCRR4A6NPCAOSO6L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L/action/storage_attestation","attest_author":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L/action/author_attestation","sign_citation":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L/action/citation_signature","submit_replication":"https://pith.science/pith/VNC3RMQT5VFCRR4A6NPCAOSO6L/action/replication_record"}},"created_at":"2026-07-05T01:07:06.075236+00:00","updated_at":"2026-07-05T01:07:06.075236+00:00"}