{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:W62BSC23IPFBRMDIB3ST3AY7HH","short_pith_number":"pith:W62BSC23","schema_version":"1.0","canonical_sha256":"b7b4190b5b43ca18b0680ee53d831f39d2f3e2b7e24d5f3a2452ab4b4e6c4251","source":{"kind":"arxiv","id":"2412.17781","version":1},"attestation_state":"computed","paper":{"title":"Variational Quantum Simulation of Anyonic Chains","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"quant-ph","authors_text":"Ananda Roy","submitted_at":"2024-12-23T18:39:28Z","abstract_excerpt":"Anyonic chains provide lattice realizations of a rich set of quantum field theories in two space-time dimensions. The latter play a central role in the investigation of generalized symmetries, renormalization group flows and numerous exotic phases of strongly-correlated systems. Here, a variational quantum simulation scheme is presented for the analysis of those anyonic chains which can be mapped to the restricted solid-on-solid~(RSOS) models of Andrews, Baxter and Forrester. An~$L_R$ site RSOS model associated with a Dynkin diagram containing~$p$ nodes is realized with~$L_R\\lceil\\ln_2 p\\rceil"},"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":"2412.17781","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-12-23T18:39:28Z","cross_cats_sorted":["hep-th","math-ph","math.MP"],"title_canon_sha256":"cf2a6d73528f21be477af2744278cb2bb23107e49d2f316cfbeac10db299b28c","abstract_canon_sha256":"d42a974e9cf040b33a629571d190f29262f2020ed8067433001cce1e2a3575e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:53:27.240425Z","signature_b64":"OufBzCsHGYNJC3nDwdbYudBmPQv5vfM4jWC/pAGujveCwnyXSylorGkmeDFaq620rNX1bvX725BKN+sXNTBwDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7b4190b5b43ca18b0680ee53d831f39d2f3e2b7e24d5f3a2452ab4b4e6c4251","last_reissued_at":"2026-07-05T09:53:27.239903Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:53:27.239903Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Variational Quantum Simulation of Anyonic Chains","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP"],"primary_cat":"quant-ph","authors_text":"Ananda Roy","submitted_at":"2024-12-23T18:39:28Z","abstract_excerpt":"Anyonic chains provide lattice realizations of a rich set of quantum field theories in two space-time dimensions. The latter play a central role in the investigation of generalized symmetries, renormalization group flows and numerous exotic phases of strongly-correlated systems. Here, a variational quantum simulation scheme is presented for the analysis of those anyonic chains which can be mapped to the restricted solid-on-solid~(RSOS) models of Andrews, Baxter and Forrester. An~$L_R$ site RSOS model associated with a Dynkin diagram containing~$p$ nodes is realized with~$L_R\\lceil\\ln_2 p\\rceil"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.17781","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/2412.17781/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":"2412.17781","created_at":"2026-07-05T09:53:27.239969+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.17781v1","created_at":"2026-07-05T09:53:27.239969+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.17781","created_at":"2026-07-05T09:53:27.239969+00:00"},{"alias_kind":"pith_short_12","alias_value":"W62BSC23IPFB","created_at":"2026-07-05T09:53:27.239969+00:00"},{"alias_kind":"pith_short_16","alias_value":"W62BSC23IPFBRMDI","created_at":"2026-07-05T09:53:27.239969+00:00"},{"alias_kind":"pith_short_8","alias_value":"W62BSC23","created_at":"2026-07-05T09:53:27.239969+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.25999","citing_title":"Lattice Topological Defects in Non-Unitary Conformal Field Theories","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH","json":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH.json","graph_json":"https://pith.science/api/pith-number/W62BSC23IPFBRMDIB3ST3AY7HH/graph.json","events_json":"https://pith.science/api/pith-number/W62BSC23IPFBRMDIB3ST3AY7HH/events.json","paper":"https://pith.science/paper/W62BSC23"},"agent_actions":{"view_html":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH","download_json":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH.json","view_paper":"https://pith.science/paper/W62BSC23","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.17781&json=true","fetch_graph":"https://pith.science/api/pith-number/W62BSC23IPFBRMDIB3ST3AY7HH/graph.json","fetch_events":"https://pith.science/api/pith-number/W62BSC23IPFBRMDIB3ST3AY7HH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH/action/storage_attestation","attest_author":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH/action/author_attestation","sign_citation":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH/action/citation_signature","submit_replication":"https://pith.science/pith/W62BSC23IPFBRMDIB3ST3AY7HH/action/replication_record"}},"created_at":"2026-07-05T09:53:27.239969+00:00","updated_at":"2026-07-05T09:53:27.239969+00:00"}