{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:B6KIFYVXSWXEY2B3A4HYZIH46Z","short_pith_number":"pith:B6KIFYVX","canonical_record":{"source":{"id":"1706.10233","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-30T15:04:12Z","cross_cats_sorted":[],"title_canon_sha256":"2426ffbb1d14a2885dbd5562eee560bd012bb82afb01a9620881023b0f605ef4","abstract_canon_sha256":"4a3f7f7a7b232b305cce692cf9a5332af12fbf51a27fa1e1df556fe3064f1091"},"schema_version":"1.0"},"canonical_sha256":"0f9482e2b795ae4c683b070f8ca0fcf665c2504df52504429d19355c81d0d1e2","source":{"kind":"arxiv","id":"1706.10233","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.10233","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"arxiv_version","alias_value":"1706.10233v2","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.10233","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"pith_short_12","alias_value":"B6KIFYVXSWXE","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"B6KIFYVXSWXEY2B3","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"B6KIFYVX","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:B6KIFYVXSWXEY2B3A4HYZIH46Z","target":"record","payload":{"canonical_record":{"source":{"id":"1706.10233","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-30T15:04:12Z","cross_cats_sorted":[],"title_canon_sha256":"2426ffbb1d14a2885dbd5562eee560bd012bb82afb01a9620881023b0f605ef4","abstract_canon_sha256":"4a3f7f7a7b232b305cce692cf9a5332af12fbf51a27fa1e1df556fe3064f1091"},"schema_version":"1.0"},"canonical_sha256":"0f9482e2b795ae4c683b070f8ca0fcf665c2504df52504429d19355c81d0d1e2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:34:34.844517Z","signature_b64":"NIcPWuTV9pOeLlSIVjpLphMnf9Vsq8QUu3cluWMNUxJii7Yt8N4dd9V0lMJxq9dmhWY7VWadGeWIywNngef2BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0f9482e2b795ae4c683b070f8ca0fcf665c2504df52504429d19355c81d0d1e2","last_reissued_at":"2026-05-18T00:34:34.844124Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:34:34.844124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.10233","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:34:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2oQgmKlKQqfmgytwwlK5anny1so4v+ttGHUQJzZ+eWlbypcYzSxYqmXPS4ufumbwagLcrEzwKDwantz/HCIaCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T08:30:05.127687Z"},"content_sha256":"fdf1678c6a2005afc2a10020e5a510468a470583b212302797035ed9633c2d01","schema_version":"1.0","event_id":"sha256:fdf1678c6a2005afc2a10020e5a510468a470583b212302797035ed9633c2d01"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:B6KIFYVXSWXEY2B3A4HYZIH46Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conservation in two-particle self-consistent extensions of dynamical-mean-field-theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. I. Lichtenstein, E. G. C. P. van Loon, F. Krien, H. Hafermann, J. Otsuki, M. I. Katsnelson","submitted_at":"2017-06-30T15:04:12Z","abstract_excerpt":"Extensions of dynamical-mean-field-theory (DMFT) make use of quantum impurity models as non-perturbative and exactly solvable reference systems which are essential to treat the strong electronic correlations. Through the introduction of retarded interactions on the impurity, these approximations can be made two-particle self-consistent. This is of interest for the Hubbard model, because it allows to suppress the antiferromagnetic phase transition in two-dimensions in accordance with the Mermin-Wagner theorem, and to include the effects of bosonic fluctuations. For a physically sound descriptio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.10233","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":""},"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":"2026-05-18T00:34:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EeVN2F9P7lP6UDQOOzqomlodS/rCZcB/LQYmsj8sfNGkQy/NEYcjCKJNcsadn+ZJQ7ryWhFEjs9kUaJ7ogY2BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T08:30:05.128352Z"},"content_sha256":"e9591f17d742b08b1a0fa08539c40e49807c45bf42d4f933428a60effb369ad5","schema_version":"1.0","event_id":"sha256:e9591f17d742b08b1a0fa08539c40e49807c45bf42d4f933428a60effb369ad5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/bundle.json","state_url":"https://pith.science/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/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":"2026-05-25T08:30:05Z","links":{"resolver":"https://pith.science/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z","bundle":"https://pith.science/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/bundle.json","state":"https://pith.science/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B6KIFYVXSWXEY2B3A4HYZIH46Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:B6KIFYVXSWXEY2B3A4HYZIH46Z","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":"4a3f7f7a7b232b305cce692cf9a5332af12fbf51a27fa1e1df556fe3064f1091","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-30T15:04:12Z","title_canon_sha256":"2426ffbb1d14a2885dbd5562eee560bd012bb82afb01a9620881023b0f605ef4"},"schema_version":"1.0","source":{"id":"1706.10233","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.10233","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"arxiv_version","alias_value":"1706.10233v2","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.10233","created_at":"2026-05-18T00:34:34Z"},{"alias_kind":"pith_short_12","alias_value":"B6KIFYVXSWXE","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"B6KIFYVXSWXEY2B3","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"B6KIFYVX","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:e9591f17d742b08b1a0fa08539c40e49807c45bf42d4f933428a60effb369ad5","target":"graph","created_at":"2026-05-18T00:34:34Z","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":"Extensions of dynamical-mean-field-theory (DMFT) make use of quantum impurity models as non-perturbative and exactly solvable reference systems which are essential to treat the strong electronic correlations. Through the introduction of retarded interactions on the impurity, these approximations can be made two-particle self-consistent. This is of interest for the Hubbard model, because it allows to suppress the antiferromagnetic phase transition in two-dimensions in accordance with the Mermin-Wagner theorem, and to include the effects of bosonic fluctuations. For a physically sound descriptio","authors_text":"A. I. Lichtenstein, E. G. C. P. van Loon, F. Krien, H. Hafermann, J. Otsuki, M. I. Katsnelson","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-30T15:04:12Z","title":"Conservation in two-particle self-consistent extensions of dynamical-mean-field-theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.10233","kind":"arxiv","version":2},"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:fdf1678c6a2005afc2a10020e5a510468a470583b212302797035ed9633c2d01","target":"record","created_at":"2026-05-18T00:34:34Z","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":"4a3f7f7a7b232b305cce692cf9a5332af12fbf51a27fa1e1df556fe3064f1091","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-30T15:04:12Z","title_canon_sha256":"2426ffbb1d14a2885dbd5562eee560bd012bb82afb01a9620881023b0f605ef4"},"schema_version":"1.0","source":{"id":"1706.10233","kind":"arxiv","version":2}},"canonical_sha256":"0f9482e2b795ae4c683b070f8ca0fcf665c2504df52504429d19355c81d0d1e2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0f9482e2b795ae4c683b070f8ca0fcf665c2504df52504429d19355c81d0d1e2","first_computed_at":"2026-05-18T00:34:34.844124Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:34:34.844124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NIcPWuTV9pOeLlSIVjpLphMnf9Vsq8QUu3cluWMNUxJii7Yt8N4dd9V0lMJxq9dmhWY7VWadGeWIywNngef2BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:34:34.844517Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.10233","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fdf1678c6a2005afc2a10020e5a510468a470583b212302797035ed9633c2d01","sha256:e9591f17d742b08b1a0fa08539c40e49807c45bf42d4f933428a60effb369ad5"],"state_sha256":"ac260cbd724a896e3b511e1ef06f8b20ea4eebca83fa413c59779d71e5fcf035"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ft6OKZPU4OPAKe6mSYw2X5yrcZ0PJS9nzU5tnKTQmx6eFC3NLMuIs1OmkzckH/vT8PX8FIcyv/bhC9OEUB91Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T08:30:05.131877Z","bundle_sha256":"702ca6aa4447e01781485cf65ff8aa6ada611dafa0e552d2d2c94ca150c1b618"}}