{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ZO4LF2IHP3JMSGRP35HTUY4J4Y","short_pith_number":"pith:ZO4LF2IH","schema_version":"1.0","canonical_sha256":"cbb8b2e9077ed2c91a2fdf4f3a6389e63993ce4302bc9f1b446b86b24c245fbd","source":{"kind":"arxiv","id":"2411.11535","version":2},"attestation_state":"computed","paper":{"title":"Universal solution to the Schrieffer-Wolff Transformation Generator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"quant-ph","authors_text":"Giovanni Francesco Diotallevi, Leander Reascos, M\\'onica Benito","submitted_at":"2024-11-18T12:46:57Z","abstract_excerpt":"The Schrieffer-Wolff transformation (SWT) is an important perturbative method in quantum mechanics used to simplify Hamiltonians by decoupling low- and high-energy subspaces. Existing methods for implementing the SWT often lack general applicability to arbitrary perturbative systems or fail to provide a closed-form solution for the SWT generator. In this article, we present a systematic and unified framework for the SWT that addresses these shortcomings. Specifically, we derive a closed-form solution for the SWT generator that is universally applicable to any system that satisfies the conditio"},"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":"2411.11535","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-11-18T12:46:57Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"a321c5d9da940171934be7322fd4b7d01f1cc1b68f8794acc527c2cc0d903926","abstract_canon_sha256":"71e9e140417df4f0fee2e61af96ddedc20407b437d730fbbbe18515010dfbdb7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:23:19.774378Z","signature_b64":"smDrvgelWr0RwPsr43A1LDZ458rfsWhc+Jo1en3JFsCdU6q9bp5EDja/AY/b3A2/MsGv3qhFWX67aWMXkH3EDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cbb8b2e9077ed2c91a2fdf4f3a6389e63993ce4302bc9f1b446b86b24c245fbd","last_reissued_at":"2026-07-05T11:23:19.773908Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:23:19.773908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal solution to the Schrieffer-Wolff Transformation Generator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"quant-ph","authors_text":"Giovanni Francesco Diotallevi, Leander Reascos, M\\'onica Benito","submitted_at":"2024-11-18T12:46:57Z","abstract_excerpt":"The Schrieffer-Wolff transformation (SWT) is an important perturbative method in quantum mechanics used to simplify Hamiltonians by decoupling low- and high-energy subspaces. Existing methods for implementing the SWT often lack general applicability to arbitrary perturbative systems or fail to provide a closed-form solution for the SWT generator. In this article, we present a systematic and unified framework for the SWT that addresses these shortcomings. Specifically, we derive a closed-form solution for the SWT generator that is universally applicable to any system that satisfies the conditio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.11535","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/2411.11535/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":"2411.11535","created_at":"2026-07-05T11:23:19.773964+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.11535v2","created_at":"2026-07-05T11:23:19.773964+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.11535","created_at":"2026-07-05T11:23:19.773964+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZO4LF2IHP3JM","created_at":"2026-07-05T11:23:19.773964+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZO4LF2IHP3JMSGRP","created_at":"2026-07-05T11:23:19.773964+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZO4LF2IH","created_at":"2026-07-05T11:23:19.773964+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.03019","citing_title":"State Specific Measurement Protocols for the Variational Quantum Eigensolver","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y","json":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y.json","graph_json":"https://pith.science/api/pith-number/ZO4LF2IHP3JMSGRP35HTUY4J4Y/graph.json","events_json":"https://pith.science/api/pith-number/ZO4LF2IHP3JMSGRP35HTUY4J4Y/events.json","paper":"https://pith.science/paper/ZO4LF2IH"},"agent_actions":{"view_html":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y","download_json":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y.json","view_paper":"https://pith.science/paper/ZO4LF2IH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.11535&json=true","fetch_graph":"https://pith.science/api/pith-number/ZO4LF2IHP3JMSGRP35HTUY4J4Y/graph.json","fetch_events":"https://pith.science/api/pith-number/ZO4LF2IHP3JMSGRP35HTUY4J4Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y/action/storage_attestation","attest_author":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y/action/author_attestation","sign_citation":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y/action/citation_signature","submit_replication":"https://pith.science/pith/ZO4LF2IHP3JMSGRP35HTUY4J4Y/action/replication_record"}},"created_at":"2026-07-05T11:23:19.773964+00:00","updated_at":"2026-07-05T11:23:19.773964+00:00"}