{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:EPN2F6K4BE3A4VGMVSJTQDIGVD","short_pith_number":"pith:EPN2F6K4","schema_version":"1.0","canonical_sha256":"23dba2f95c09360e54ccac93380d06a8cce49992f6cbf650d0d909fbb6612965","source":{"kind":"arxiv","id":"2507.03092","version":2},"attestation_state":"computed","paper":{"title":"STABSim: A Parallelized Clifford Simulator with Features Beyond Direct Simulation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ang Li, Chenxu Liu, Meng Wang, Samuel Stein, Sean Garner","submitted_at":"2025-07-03T18:05:19Z","abstract_excerpt":"The quantum stabilizer formalism became foundational for understanding error correction soon after the realization of the first useful quantum error correction codes. Stabilizers provide a way to describe sets of quantum states which are valid codewords within a quantum error correction (QEC) scheme. Existing stabilizer simulators are single threaded applications used to sample larger codes than is possible with other methods. However, there is an outstanding gap in the scaling and accuracy of current simulators for QEC as quantum computing exceeds hundreds of qubits, along with an under-utili"},"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":"2507.03092","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-07-03T18:05:19Z","cross_cats_sorted":[],"title_canon_sha256":"013d8fd8433ad0bdf1f2203d6b2b925dfc7f5e2437bc479896443379a3948706","abstract_canon_sha256":"477f8d61f12020825810ac7b1318480d50012383cb5f718c7d5c4036005357de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:57:20.619821Z","signature_b64":"M4GOyQFvR3yjp5pgTtfKPCsUcW9K1sAlqa5MBx5JLi7F2nmdmKYoETlnxnI+4xyDfZVS4V/ickmrouX4bP36Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23dba2f95c09360e54ccac93380d06a8cce49992f6cbf650d0d909fbb6612965","last_reissued_at":"2026-07-05T11:57:20.619300Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:57:20.619300Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"STABSim: A Parallelized Clifford Simulator with Features Beyond Direct Simulation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Ang Li, Chenxu Liu, Meng Wang, Samuel Stein, Sean Garner","submitted_at":"2025-07-03T18:05:19Z","abstract_excerpt":"The quantum stabilizer formalism became foundational for understanding error correction soon after the realization of the first useful quantum error correction codes. Stabilizers provide a way to describe sets of quantum states which are valid codewords within a quantum error correction (QEC) scheme. Existing stabilizer simulators are single threaded applications used to sample larger codes than is possible with other methods. However, there is an outstanding gap in the scaling and accuracy of current simulators for QEC as quantum computing exceeds hundreds of qubits, along with an under-utili"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.03092","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2507.03092/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":"2507.03092","created_at":"2026-07-05T11:57:20.619384+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.03092v2","created_at":"2026-07-05T11:57:20.619384+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.03092","created_at":"2026-07-05T11:57:20.619384+00:00"},{"alias_kind":"pith_short_12","alias_value":"EPN2F6K4BE3A","created_at":"2026-07-05T11:57:20.619384+00:00"},{"alias_kind":"pith_short_16","alias_value":"EPN2F6K4BE3A4VGM","created_at":"2026-07-05T11:57:20.619384+00:00"},{"alias_kind":"pith_short_8","alias_value":"EPN2F6K4","created_at":"2026-07-05T11:57:20.619384+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.25974","citing_title":"PauLIB: A High-Performance Library for Processing Pauli Strings","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2512.09189","citing_title":"Exact and Efficient Stabilizer Simulation of Thermal-Relaxation Noise for Quantum Error Correction","ref_index":62,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04049","citing_title":"FTPrimitiveBench: A Benchmark Suite For Logical Computation Under Hardware-Motivated and Biased Noise Models","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD","json":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD.json","graph_json":"https://pith.science/api/pith-number/EPN2F6K4BE3A4VGMVSJTQDIGVD/graph.json","events_json":"https://pith.science/api/pith-number/EPN2F6K4BE3A4VGMVSJTQDIGVD/events.json","paper":"https://pith.science/paper/EPN2F6K4"},"agent_actions":{"view_html":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD","download_json":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD.json","view_paper":"https://pith.science/paper/EPN2F6K4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.03092&json=true","fetch_graph":"https://pith.science/api/pith-number/EPN2F6K4BE3A4VGMVSJTQDIGVD/graph.json","fetch_events":"https://pith.science/api/pith-number/EPN2F6K4BE3A4VGMVSJTQDIGVD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD/action/storage_attestation","attest_author":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD/action/author_attestation","sign_citation":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD/action/citation_signature","submit_replication":"https://pith.science/pith/EPN2F6K4BE3A4VGMVSJTQDIGVD/action/replication_record"}},"created_at":"2026-07-05T11:57:20.619384+00:00","updated_at":"2026-07-05T11:57:20.619384+00:00"}