{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JZGCNCK26EHDV5TZJ3HLMEECOS","short_pith_number":"pith:JZGCNCK2","schema_version":"1.0","canonical_sha256":"4e4c26895af10e3af6794eceb6108274bfcc06b7e1fc5fb8ec1716f230098354","source":{"kind":"arxiv","id":"2408.12641","version":1},"attestation_state":"computed","paper":{"title":"Surrogate Constructed Scalable Circuits ADAPT-VQE in the Schwinger model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"quant-ph","authors_text":"Adrien Florio, Andreas Weichselbaum, Erik Gustafson, Henry Lamm, Karunya Shirali, Kyle Sherbert, Norm M. Tubman, Robert D. Pisarski, Semeon Valgushev, Sophia E. Economou, Yanzhu Chen","submitted_at":"2024-08-22T18:00:00Z","abstract_excerpt":"Inspired by recent advancements of simulating periodic systems on quantum computers, we develop a new approach, (SC)$^2$-ADAPT-VQE, to further advance the simulation of these systems. Our approach extends the scalable circuits ADAPT-VQE framework, which builds an ansatz from a pool of coordinate-invariant operators defined for arbitrarily large, though not arbitrarily small, volumes. Our method uses a classically tractable ``Surrogate Constructed'' method to remove irrelevant operators from the pool, reducing the minimum size for which the scalable circuits are defined. Bringing together the s"},"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":"2408.12641","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-08-22T18:00:00Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"523cf3ee0e82fc787d2c5fdc8f64184df2ce6b11e64f1beb8f0136425f0f5450","abstract_canon_sha256":"2c2d282a8d0fa387ed3968eb472ffa72e9dd17ce0ad1c96a1f1838607799e316"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:58:27.839123Z","signature_b64":"W+rNYWJaojVfdjeboTzxjVCLtapFkxxwOMmqrvPb47UpUbyVFUPaRaaE7jQGbT70CoBZDCwGn6j1+JoCVKN8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e4c26895af10e3af6794eceb6108274bfcc06b7e1fc5fb8ec1716f230098354","last_reissued_at":"2026-07-05T08:58:27.838691Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:58:27.838691Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Surrogate Constructed Scalable Circuits ADAPT-VQE in the Schwinger model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"quant-ph","authors_text":"Adrien Florio, Andreas Weichselbaum, Erik Gustafson, Henry Lamm, Karunya Shirali, Kyle Sherbert, Norm M. Tubman, Robert D. Pisarski, Semeon Valgushev, Sophia E. Economou, Yanzhu Chen","submitted_at":"2024-08-22T18:00:00Z","abstract_excerpt":"Inspired by recent advancements of simulating periodic systems on quantum computers, we develop a new approach, (SC)$^2$-ADAPT-VQE, to further advance the simulation of these systems. Our approach extends the scalable circuits ADAPT-VQE framework, which builds an ansatz from a pool of coordinate-invariant operators defined for arbitrarily large, though not arbitrarily small, volumes. Our method uses a classically tractable ``Surrogate Constructed'' method to remove irrelevant operators from the pool, reducing the minimum size for which the scalable circuits are defined. Bringing together the s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.12641","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/2408.12641/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":"2408.12641","created_at":"2026-07-05T08:58:27.838747+00:00"},{"alias_kind":"arxiv_version","alias_value":"2408.12641v1","created_at":"2026-07-05T08:58:27.838747+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.12641","created_at":"2026-07-05T08:58:27.838747+00:00"},{"alias_kind":"pith_short_12","alias_value":"JZGCNCK26EHD","created_at":"2026-07-05T08:58:27.838747+00:00"},{"alias_kind":"pith_short_16","alias_value":"JZGCNCK26EHDV5TZ","created_at":"2026-07-05T08:58:27.838747+00:00"},{"alias_kind":"pith_short_8","alias_value":"JZGCNCK2","created_at":"2026-07-05T08:58:27.838747+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.05297","citing_title":"Continuous-variable ADAPT-VQE for bosonic lattice models","ref_index":76,"is_internal_anchor":false},{"citing_arxiv_id":"2512.05210","citing_title":"A Framework for Quantum Simulations of Energy-Loss and Hadronization in Non-Abelian Gauge Theories: SU(2) Lattice Gauge Theory in 1+1D","ref_index":134,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS","json":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS.json","graph_json":"https://pith.science/api/pith-number/JZGCNCK26EHDV5TZJ3HLMEECOS/graph.json","events_json":"https://pith.science/api/pith-number/JZGCNCK26EHDV5TZJ3HLMEECOS/events.json","paper":"https://pith.science/paper/JZGCNCK2"},"agent_actions":{"view_html":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS","download_json":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS.json","view_paper":"https://pith.science/paper/JZGCNCK2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2408.12641&json=true","fetch_graph":"https://pith.science/api/pith-number/JZGCNCK26EHDV5TZJ3HLMEECOS/graph.json","fetch_events":"https://pith.science/api/pith-number/JZGCNCK26EHDV5TZJ3HLMEECOS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS/action/storage_attestation","attest_author":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS/action/author_attestation","sign_citation":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS/action/citation_signature","submit_replication":"https://pith.science/pith/JZGCNCK26EHDV5TZJ3HLMEECOS/action/replication_record"}},"created_at":"2026-07-05T08:58:27.838747+00:00","updated_at":"2026-07-05T08:58:27.838747+00:00"}