{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:6T2HRPHTL3MCN3U54EMD2OLJ22","short_pith_number":"pith:6T2HRPHT","canonical_record":{"source":{"id":"1604.08138","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-27T16:49:02Z","cross_cats_sorted":[],"title_canon_sha256":"a13a5d2f7e845eeb5b601fd2bbcd4f80cd30cecf6d0bd576fbc73a75b9a577c5","abstract_canon_sha256":"22bbe41c64700f6f50111ea5bbcc74e7822b5bbfc20322a28dcb642d35e87192"},"schema_version":"1.0"},"canonical_sha256":"f4f478bcf35ed826ee9de1183d3969d6a0ea6c12e0a486eaf57c31cb728c4bb8","source":{"kind":"arxiv","id":"1604.08138","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.08138","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"arxiv_version","alias_value":"1604.08138v1","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08138","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"pith_short_12","alias_value":"6T2HRPHTL3MC","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6T2HRPHTL3MCN3U5","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6T2HRPHT","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:6T2HRPHTL3MCN3U54EMD2OLJ22","target":"record","payload":{"canonical_record":{"source":{"id":"1604.08138","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-27T16:49:02Z","cross_cats_sorted":[],"title_canon_sha256":"a13a5d2f7e845eeb5b601fd2bbcd4f80cd30cecf6d0bd576fbc73a75b9a577c5","abstract_canon_sha256":"22bbe41c64700f6f50111ea5bbcc74e7822b5bbfc20322a28dcb642d35e87192"},"schema_version":"1.0"},"canonical_sha256":"f4f478bcf35ed826ee9de1183d3969d6a0ea6c12e0a486eaf57c31cb728c4bb8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:23.407570Z","signature_b64":"nidNYub8aAswAQXt9foc+DOLYXD1XCXD61Wyu2fT+scgDx6ACjrsWJiODJgrnARJmX8cCAJqp0VDdEtsIxisCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4f478bcf35ed826ee9de1183d3969d6a0ea6c12e0a486eaf57c31cb728c4bb8","last_reissued_at":"2026-05-18T00:52:23.406908Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:23.406908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.08138","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:52:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yRGriBQni8CbuY4JV8jVe0BwM7um0M8/exRol006xu1/VkgCXTY6gIxFr29M/JPwvUA+pNUk+piXuVgEmKNaCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:27:37.926378Z"},"content_sha256":"2434b981753f40d4928b66d8631a9093f8806222010f60bbd8ddd63f2269ba59","schema_version":"1.0","event_id":"sha256:2434b981753f40d4928b66d8631a9093f8806222010f60bbd8ddd63f2269ba59"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:6T2HRPHTL3MCN3U54EMD2OLJ22","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dual-fermion approach to the Anderson-Hubbard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"J. Moreno, M. Jarrell, P. Haase, S.-X. Yang, T. Pruschke","submitted_at":"2016-04-27T16:49:02Z","abstract_excerpt":"We apply the recently developed dual fermion algorithm for disordered interacting systems to the Anderson-Hubbard model. This algorithm is compared with dynamical cluster approximation calculations for a one-dimensional system to establish the quality of the approximation in comparison with an established cluster method. We continue with a three-dimensional (3d) system and look at the antiferromagnetic, Mott and Anderson localization transitions. The dual fermion approach leads to quantitative as well as qualitative improvement of the dynamical mean-field results and it allows one to calculate"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08138","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:52:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tFkH8lfUHYX5zaEZtmPuanrfm/cIOoZbjYt6nsqiN8IXTe5lqj+Rif+Yn2G/x6xe29Wolw84KfF9teWy/hU9DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:27:37.926735Z"},"content_sha256":"384c3c2ad6a1f3b1201296a025d537691d283db71b24ece6f3924dfc825b988e","schema_version":"1.0","event_id":"sha256:384c3c2ad6a1f3b1201296a025d537691d283db71b24ece6f3924dfc825b988e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/bundle.json","state_url":"https://pith.science/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T01:27:37Z","links":{"resolver":"https://pith.science/pith/6T2HRPHTL3MCN3U54EMD2OLJ22","bundle":"https://pith.science/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/bundle.json","state":"https://pith.science/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6T2HRPHTL3MCN3U54EMD2OLJ22/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:6T2HRPHTL3MCN3U54EMD2OLJ22","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"22bbe41c64700f6f50111ea5bbcc74e7822b5bbfc20322a28dcb642d35e87192","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-27T16:49:02Z","title_canon_sha256":"a13a5d2f7e845eeb5b601fd2bbcd4f80cd30cecf6d0bd576fbc73a75b9a577c5"},"schema_version":"1.0","source":{"id":"1604.08138","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.08138","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"arxiv_version","alias_value":"1604.08138v1","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08138","created_at":"2026-05-18T00:52:23Z"},{"alias_kind":"pith_short_12","alias_value":"6T2HRPHTL3MC","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6T2HRPHTL3MCN3U5","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6T2HRPHT","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:384c3c2ad6a1f3b1201296a025d537691d283db71b24ece6f3924dfc825b988e","target":"graph","created_at":"2026-05-18T00:52:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We apply the recently developed dual fermion algorithm for disordered interacting systems to the Anderson-Hubbard model. This algorithm is compared with dynamical cluster approximation calculations for a one-dimensional system to establish the quality of the approximation in comparison with an established cluster method. We continue with a three-dimensional (3d) system and look at the antiferromagnetic, Mott and Anderson localization transitions. The dual fermion approach leads to quantitative as well as qualitative improvement of the dynamical mean-field results and it allows one to calculate","authors_text":"J. Moreno, M. Jarrell, P. Haase, S.-X. Yang, T. Pruschke","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-27T16:49:02Z","title":"Dual-fermion approach to the Anderson-Hubbard model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08138","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2434b981753f40d4928b66d8631a9093f8806222010f60bbd8ddd63f2269ba59","target":"record","created_at":"2026-05-18T00:52:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"22bbe41c64700f6f50111ea5bbcc74e7822b5bbfc20322a28dcb642d35e87192","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-27T16:49:02Z","title_canon_sha256":"a13a5d2f7e845eeb5b601fd2bbcd4f80cd30cecf6d0bd576fbc73a75b9a577c5"},"schema_version":"1.0","source":{"id":"1604.08138","kind":"arxiv","version":1}},"canonical_sha256":"f4f478bcf35ed826ee9de1183d3969d6a0ea6c12e0a486eaf57c31cb728c4bb8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f4f478bcf35ed826ee9de1183d3969d6a0ea6c12e0a486eaf57c31cb728c4bb8","first_computed_at":"2026-05-18T00:52:23.406908Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:52:23.406908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nidNYub8aAswAQXt9foc+DOLYXD1XCXD61Wyu2fT+scgDx6ACjrsWJiODJgrnARJmX8cCAJqp0VDdEtsIxisCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:52:23.407570Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.08138","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2434b981753f40d4928b66d8631a9093f8806222010f60bbd8ddd63f2269ba59","sha256:384c3c2ad6a1f3b1201296a025d537691d283db71b24ece6f3924dfc825b988e"],"state_sha256":"b9fd8e2950126d03ed0ce70b43e9fa6513340ac33bbc01e43a2de1e437717247"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sg46KTEi1y3Aq2//fgdl6kff3obITv/mfg/hb9v91g3D8l3Z860ksp4hDZ7JSnkCiehLdI7CLRfzy2HkBWViCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T01:27:37.928874Z","bundle_sha256":"1a7233fdd743c5f572870cec2b76209935dd9bdf2dcb481853b916c5e99a333a"}}