{"as_of":"2026-08-16T07:29:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:2481a8c18151bba43d98f99040ed1aa1707357e6c3ad3f25d983001d2ee10501","coverage":[{"denominator":98,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":98,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T15:54:35.833002Z","state":"measured"},{"denominator":99,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":99,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-16T06:30:59.297886+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T04:45:59.682877Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-08-14T04:45:59.830726Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"cited_work":{"arxiv_id":"1908.00536","doi":null,"metadata_source":"pith","pith_arxiv_id":"1908.00536","snapshot_observed_at":"2026-08-14T04:45:59.830726Z","title":"Consistent partial bosonization of the extended Hubbard model","venue":"cond-mat.str-el","work_id":"6f5db2a5-c0c3-45bc-a69c-6ad016ffcc9f","year":2019},"citing_paper":{"arxiv_id":"1909.02793","last_updated":"2019-12-28T20:16:30Z","snapshot_observed_at":"2026-08-14T04:36:36.377554Z","submitted_at":"2019-09-06T09:32:20Z","title":"Parquet-like equations for the Hedin three-leg vertex","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T04:45:59.682877Z"},"links":{"cited_paper":"/paper/1908.00536","citing_paper":"/paper/1909.02793"},"observation_digest":"sha256:383e1fb0a0d02c9f5dce29cfd3a5c83bb59ae95e6f46c756f7f3a16ad8d59c01","observation_id":"d2579f05-5f66-4a48-b36b-fe3674098923","resolution":{"observed_at":"2026-08-14T04:45:59.833779Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1908.00536/citation-record","integrity":"/paper/1908.00536/integrity","json":"/paper/1908.00536/citation-record.json","paper":"/paper/1908.00536"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.472388Z","title":"Fradkin, Field Theories of Condensed Matter Systems (West- view Press, Oxford, 1997)","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.472388Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:ab7bb0693cc3118cfac1d5a5f1a0bb935236168f701299d472cd326ed594ea6a","observation_id":"78d67d89-92bc-4a4a-a8e8-decff7fc83bc","resolution":{"observed_at":"2026-08-14T15:54:35.472388Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.476558Z","title":"S ´en´echal, A","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.476558Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:2112aadf398b5a1352d81439c5d06b044adc7279f0dc432958252a0f85a22750","observation_id":"2a34ff3c-823a-4520-b469-51bb89fc809e","resolution":{"observed_at":"2026-08-14T15:54:35.476558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.480687Z","title":"Correlated electrons in high-temperature super- conductors,","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.480687Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:412547c39469c27382bbd2a7ac52df4e0c67398772d5deecaf15d11d6f46be4b","observation_id":"cb68b53c-ba74-4004-b740-4798d76896a2","resolution":{"observed_at":"2026-08-14T15:54:35.480687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.484351Z","title":"Superexchange mechanism and d-wave superconductivity,","venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.484351Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:ae8f944537ea2b492edf13f592eaa8477d995fb62a073c918f5d4f378e13ec98","observation_id":"ac0b7838-8ea8-4add-9af6-319908722ddf","resolution":{"observed_at":"2026-08-14T15:54:35.484351Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.487939Z","title":"Dynamical Model of Elemen- tary Particles Based on an Analogy with Superconductivity. I,","venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.487939Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:c4d491546ec1bbe7b7f702d9398b854c8813e7ba9619a85aeaad4ef0cc117044","observation_id":"a616175b-3827-4095-b432-21473f37af58","resolution":{"observed_at":"2026-08-14T15:54:35.487939Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.491447Z","title":"Dynamical Model of Elemen- tary Particles Based on an Analogy with Superconductivity. II,","venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.491447Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:211c708e31d9835010c6b61d4e45506ab241d8ca359ceb3997a42a51b2ea3591","observation_id":"11152d3f-9be0-410f-a71f-5fa13060c523","resolution":{"observed_at":"2026-08-14T15:54:35.491447Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.494997Z","title":"Superfluidity and superconductivity in relativistic fermion systems,","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.494997Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:93b0e675a41b897ad1265d1a8c2056f37ea9500c559823d2bd748801ea66e378","observation_id":"ede7b6c0-6857-4c08-b1b7-dbd267d3d44e","resolution":{"observed_at":"2026-08-14T15:54:35.494997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.498112Z","title":"QCD at finite baryon density: nucleon droplets and color superconduc- tivity,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.498112Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cd948dd42042f6233a060ae71017bbef4acd133f554df532a7585edcb7f0e621","observation_id":"84e93d7b-85c8-4f00-a1db-1bbfc7118d39","resolution":{"observed_at":"2026-08-14T15:54:35.498112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.500924Z","title":"Color superconductiv- ity and chiral symmetry restoration at non-zero baryon density and temperature,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.500924Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:310134cae321d9722fdf5a905ca4f7e811020c27c1cd011f3d66d38dd812e516","observation_id":"0760aaf7-0ab4-4ebd-bf77-d2a00f418e59","resolution":{"observed_at":"2026-08-14T15:54:35.500924Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.503925Z","title":"Color- flavor locking and chiral symmetry breaking in high density QCD,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.503925Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:2b31d4b5ba033401d0c8a68f7381d220398a4409e4f40aa5f5534013c3d518e8","observation_id":"a4c26304-7390-4183-86e4-748064777ac4","resolution":{"observed_at":"2026-08-14T15:54:35.503925Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.507410Z","title":"Continuity of Quark and Hadron Matter,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.507410Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:769ee57103dd34f61c5f5b41cb2b69f8b1491a1d51a6b281169e759f0d649d74","observation_id":"207ddb37-9fe7-41a3-8ac2-c9510872e6ad","resolution":{"observed_at":"2026-08-14T15:54:35.507410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.510307Z","title":"Dynamical symmetry break- ing in asymptotically free field theories,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.510307Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:a70b9f90cfb4768721987e08bf8ecffd16387c2a80dd2bb21adfa49bc2c94245","observation_id":"24a44e90-e3d5-4faf-8bee-9965f1a8a164","resolution":{"observed_at":"2026-08-14T15:54:35.510307Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.513691Z","title":"E ffective (2 +1)- dimensional field theory of fermions: fermion mass generation with Kaluza-Klein fermions and gauge field,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.513691Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:8dc3fd3c67432f9a5395dbafbdf8217671545ed7a9166c150a2c563bf4c10f20","observation_id":"81ce5640-58e1-40ea-88ef-ff04cdae8abe","resolution":{"observed_at":"2026-08-14T15:54:35.513691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.517222Z","title":"Flow equations without mean field ambiguity,","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.517222Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:27d2c08b0625d6f0b4ad028e520783423224db0aad8aaa214c6883f40f39cd7e","observation_id":"9500f21c-fb68-45a5-993e-73bdd13e767a","resolution":{"observed_at":"2026-08-14T15:54:35.517222Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.520571Z","title":"Temperature dependence of antiferromagnetic order in the Hubbard model,","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.520571Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:8f25fa2fc1a31351cde08f572dec81dc71d8a2d819fc7c2e2a3077e0db585f93","observation_id":"64ec110d-5b20-42b0-9775-225658ad1255","resolution":{"observed_at":"2026-08-14T15:54:35.520571Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0205154","last_updated":"2002-05-15T17:49:47Z","snapshot_observed_at":"2026-07-07T03:56:07.874456Z","submitted_at":"2002-05-15T17:49:47Z","title":"Understanding the Fierz Ambiguity of Partially Bosonized Theories","version":1},"cited_work":{"arxiv_id":"hep-ph/0205154","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0205154","snapshot_observed_at":"2026-08-14T15:54:35.950839Z","title":"Understanding the Fierz Ambiguity of Partially Bosonized Theories","venue":"hep-ph","work_id":"3c0508e8-a27c-436a-b4b6-b5d707b7255f","year":2002},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.523962Z"},"links":{"cited_paper":"/paper/hep-ph/0205154","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:37bd2ce3becaf4fcf5edfdc652279c57135b666d080340c762de95bfb475855b","observation_id":"d87a8d7c-9944-4680-8b6c-df909c2492fd","resolution":{"observed_at":"2026-08-14T15:54:35.955717Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.528002Z","title":"New Method for Calculating the One-Particle Green’s Function with Application to the Electron-Gas Prob- lem,","venue":null,"work_id":null,"year":1965},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.528002Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:34e77d6414cd5f6128fdfb063ef8d789ca299a7e6f25ae7f1b7b6171af75c3f0","observation_id":"9b498818-6c8c-4c78-889f-961d19b2f5c2","resolution":{"observed_at":"2026-08-14T15:54:35.528002Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.531372Z","title":"The GW method,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.531372Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:df88c09ddbf15c58a6cc0e86f9d246d9db4dbccb32c33b09a30f58e479658fce","observation_id":"c4795fe5-96a9-476a-ae45-9c1ac4703d36","resolution":{"observed_at":"2026-08-14T15:54:35.531372Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.535063Z","title":"On correlation e ffects in electron spectroscopies and the GW approximation,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.535063Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:3c403674b101ae42e16cee108c67875124e90d59b9e9ab1f72b3edec4b35c03f","observation_id":"4daacc67-d429-41db-8368-da3738e4e4eb","resolution":{"observed_at":"2026-08-14T15:54:35.535063Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.817877Z","title":"Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite di- mensions,","venue":null,"work_id":"85c01a85-1379-4527-bce4-af657719d9fd","year":1996},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.538537Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:43f7bf571e40557ba8b6585681432f005618d6110fb5ddd04fe226441a261a56","observation_id":"7dcb8599-f1cc-441a-b9d5-041f35a1d2e9","resolution":{"observed_at":"2026-08-14T15:54:36.822014Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.807002Z","title":"Non-Fermi-liquid behavior near a T =0 spin-glass transition,","venue":null,"work_id":"b77243f4-d981-43c7-9c39-76b6c85b88b9","year":1995},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.542780Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:49ee42c547fdb96a1a26ecbc3c61d1ddf0eeae1c96a162b89baf3372f21d8651","observation_id":"3b0e8158-36df-4e2f-8490-b277fa78a847","resolution":{"observed_at":"2026-08-14T15:54:36.810888Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.796763Z","title":"Kosterlitz-Thouless Transition and Short Range Spatial Correlations in an Extended Hubbard Model,","venue":null,"work_id":"637fccb8-25a1-4aeb-8938-e35509969b11","year":1996},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.546275Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:f9e4288cd1688142b3208ef876d99c4e2922951df4c88fdb005a1219fd1e2aee","observation_id":"4bf9a6d9-2157-4e89-a23e-0bc7e0ec1b29","resolution":{"observed_at":"2026-08-14T15:54:36.800482Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.786204Z","title":"Spatial correlations in dynamical mean- field theory,","venue":null,"work_id":"99ffa76a-99a8-4402-8db0-31608bb9e5e8","year":2000},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.550479Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:436227f0093de71b6ca9ae57760dbd3a8754e383a9c3e1751818b1a632a32acb","observation_id":"3bd4c693-79f7-4811-bfad-4f56fa1d9d49","resolution":{"observed_at":"2026-08-14T15:54:36.789959Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.774999Z","title":"Effect of Long Range Coulomb Inter- actions on the Mott Transition,","venue":null,"work_id":"526c8d6e-8431-4f84-9b27-b3b88f41e957","year":2000},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.554486Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:4d064d9338978baf6103481197a56fa9d7c69c1d5e5acd07f284efe029443f62","observation_id":"d0ef03c6-4c9e-4c90-8d59-e3f7ddabcfb9","resolution":{"observed_at":"2026-08-14T15:54:36.778948Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.764220Z","title":"E ffective-action approach to strongly correlated fermion systems,","venue":null,"work_id":"566d1723-532f-4185-9cd2-e3ef1ff57578","year":2001},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.557975Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:bcc6b0c9e8d1a6b197da4435286152d8753ad48c6b03be902b3c63a96bc4c956","observation_id":"921e10f3-e34d-4c30-a81b-c69f5bf1e3e9","resolution":{"observed_at":"2026-08-14T15:54:36.768178Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.751534Z","title":"Correlated Lattice Fermions in d =∞ Dimensions,","venue":null,"work_id":"6a9c0c7a-adf4-4595-9ad0-af770fde0abf","year":1989},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.561284Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:0eb042d7001c3358cecb5a34d8daa8ea9235d2f37d3c158b59e7b6f277cb5624","observation_id":"6ef0357e-715b-4434-9c07-19caeaa95bbd","resolution":{"observed_at":"2026-08-14T15:54:36.755937Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.739640Z","title":"On the dan- gers of partial diagrammatic summations: Benchmarks for the two-dimensional hubbard model in the weak-coupling regime,","venue":null,"work_id":"d982985e-38b5-42c3-ba8c-c8e5f01096c6","year":2015},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.564988Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:a5e76ab02cad1b977a4ca36d348b58ec945288374b0347c3a92176dac89f29b4","observation_id":"a754449f-68e5-45e9-a900-53a373adaee3","resolution":{"observed_at":"2026-08-14T15:54:36.743750Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.728813Z","title":"Diagrammatic routes to nonlocal correlations beyond dynamical mean field theory,","venue":null,"work_id":"d1fbcb45-a14a-4894-97f7-442cd2ed9ba2","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.568296Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d58cf343fd23ca59c31338c43296673677cdae57f1dc99ead5f0b178474d3f88","observation_id":"eb374a9a-a71e-41f3-80a3-ca2d305852f9","resolution":{"observed_at":"2026-08-14T15:54:36.732804Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.718167Z","title":"Magnetic Excitation Spectra in BaFe 2As2: A Two-Particle Approach within a Combination of the Density Functional Theory and the Dynamical Mean-Field Theory Method,","venue":null,"work_id":"d9fed95e-eab0-4d62-9f96-82ae6fef14d3","year":2011},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.571684Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:76cbb93943082211f83dc719f80fc50ede48329286e28422be4853ebe3e0ed76","observation_id":"7a03f634-f9e7-457b-ad22-ac7a5af33ac2","resolution":{"observed_at":"2026-08-14T15:54:36.722020Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.707107Z","title":"Competing orders in Na xCoO2 from strong correlations on a two-particle level,","venue":null,"work_id":"9433b263-9bcb-4041-b2b3-c9bfe69782b5","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.575118Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:e84834697af2cd3397b4a28d753fdafadb9b5fd762976a811d2e03406a8332e0","observation_id":"dcac6cb9-e33f-47d2-a6f6-d8b2343f3588","resolution":{"observed_at":"2026-08-14T15:54:36.711571Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.696583Z","title":"Ab initio dynamical vertex approxi- mation,","venue":null,"work_id":"8fa6bad3-e4ab-4d98-ad2c-c17ec0cacd29","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.578499Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:498f7978ebfec7975a9c0a3eb90564a928f399f26ea0c5bc6cb6d34b27783e09","observation_id":"a2b343cb-dd86-43c6-99b4-c6c8a389b371","resolution":{"observed_at":"2026-08-14T15:54:36.700248Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.683474Z","title":"Multi-orbital nature of the spin fluctuations in Sr2RuO4,","venue":null,"work_id":"1cbabaa8-d4b1-4440-b881-969fe1208556","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.581879Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cbd6e2982751dadc23f91942c645aaa0bfc7690119b78be7fe363fc9463a5c25","observation_id":"981349ca-4ab0-436e-b9b8-1d4dccd423db","resolution":{"observed_at":"2026-08-14T15:54:36.687296Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.05143","last_updated":"2019-09-06T17:15:49Z","snapshot_observed_at":"2026-08-14T18:00:11.634523Z","submitted_at":"2018-11-13T07:40:03Z","title":"Evening out the spin and charge parity to increase T$_c$ in unconventional superconductor Sr_{2}RuO_{4}","version":3},"cited_work":{"arxiv_id":"1811.05143","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.05143","snapshot_observed_at":"2026-08-14T15:54:35.935369Z","title":"Evening out the spin and charge parity to increase T$_c$ in unconventional superconductor Sr_{2}RuO_{4}","venue":"cond-mat.str-el","work_id":"0cc1799c-7b02-4087-8196-645fd3b75a0c","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.585475Z"},"links":{"cited_paper":"/paper/1811.05143","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d21a3911b5949106ddd846c9f883ff318f7661865e3638449f1b3b4e527cc680","observation_id":"7d379f4c-081b-4cd6-ae5e-c7670f36fc83","resolution":{"observed_at":"2026-08-14T15:54:35.939919Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1904.07324","last_updated":"2019-04-15T20:35:58Z","snapshot_observed_at":"2026-08-14T16:46:09.589962Z","submitted_at":"2019-04-15T20:35:58Z","title":"Magnetic response of Sr$_2$RuO$_4$: quasi-local spin fluctuations due to Hund's coupling","version":1},"cited_work":{"arxiv_id":"1904.07324","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.07324","snapshot_observed_at":"2026-08-14T15:54:35.919990Z","title":"Magnetic response of Sr$_2$RuO$_4$: quasi-local spin fluctuations due to Hund's coupling","venue":"cond-mat.str-el","work_id":"e234bbb1-923e-4e96-aba4-5060309ccdb4","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.589442Z"},"links":{"cited_paper":"/paper/1904.07324","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:052a479a29e20f211393d45cac35822d04896dca352cbb9c27bd22e715a1d963","observation_id":"12db1b6a-04d6-4ae3-893e-75f823ff9157","resolution":{"observed_at":"2026-08-14T15:54:35.924177Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.672146Z","title":"Extended dynamical mean-field theory and GW method,","venue":null,"work_id":"4ef1eb4b-ddee-4146-bbf9-ddae08303ea5","year":2002},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.593647Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d5889dfb593662fd760ee03dd54e4c3d57b3ba02d92138362f5cf47b7978e41c","observation_id":"5b20b8ca-ec02-4d8c-b7eb-101809220a43","resolution":{"observed_at":"2026-08-14T15:54:36.676170Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.660129Z","title":"First- Principles Approach to the Electronic Structure of Strongly Correlated Systems: Combining the GW Approximation and Dynamical Mean-Field Theory,","venue":null,"work_id":"6d86c3ff-4bf3-41c4-8c19-7d9ae688a5f5","year":2003},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.597362Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:028a9d64935756918b68e31826e40ef4dcafe382c838a384c5a5a9d38dde3bf9","observation_id":"b29531d2-7c5f-4f2f-a19f-bc01ec354848","resolution":{"observed_at":"2026-08-14T15:54:36.664743Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.646203Z","title":"Spectral Properties of Correlated Materials: Local Vertex and Nonlocal Two-Particle Correlations from Combined GW and Dynamical Mean Field Theory,","venue":null,"work_id":"0563a0d1-4136-41d0-bd35-82c937a692be","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.600219Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:94ca5fd1313649954316ca8dd852f9d44a250af4c703a85f73dcbd5167a41103","observation_id":"9dfc3522-0661-415c-b4d1-6c01f45dbd93","resolution":{"observed_at":"2026-08-14T15:54:36.650747Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.635448Z","title":"Screen- ing and nonlocal correlations in the extended Hubbard model from self-consistent combined GW and dynamical mean field theory,","venue":null,"work_id":"7a913b36-f7ad-4124-93c4-6ff488f6367a","year":2013},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.603314Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:19e7ced2ac9c07073eb25ec3b46d6672666b1f381a2e6e47ee8c3f82f8269c02","observation_id":"a9e2c76d-fec1-4932-8f61-fb5f17509164","resolution":{"observed_at":"2026-08-14T15:54:36.639323Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.624240Z","title":"Extended dynamical mean-field study of the Hubbard model with long-range interactions,","venue":null,"work_id":"26ba3059-bc9b-4fd5-aa22-62ea1225c028","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.606258Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:22e5e2502cf46736ea8b0f9912580907a272ff32815f43c695b68a82f337562d","observation_id":"e31f861a-2831-4836-9569-d46a4b679b42","resolution":{"observed_at":"2026-08-14T15:54:36.628273Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.613485Z","title":"When strong correlations become weak: Consistent merging of GW and DMFT,","venue":null,"work_id":"6254c20c-17d3-4611-ac69-05740d8a0fec","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.609553Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:884e45c712ba7552264d2857cc32494c5b780e41604fcb368850b250b545fd09","observation_id":"a9a57ea6-b0eb-43a4-aeb2-1b701e1ca1fb","resolution":{"observed_at":"2026-08-14T15:54:36.617327Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.602828Z","title":"Influence of Fock exchange in combined many-body perturbation and dynamical mean field theory,","venue":null,"work_id":"cc0bff58-76c1-468e-a510-901563ac1449","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.612405Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:32ec80f57530b4fc41747a07d2dcbcb5f65b1d7f3f2f83564187c988f1f79963","observation_id":"07ca0237-2806-4f7c-b54f-4faf86cf58da","resolution":{"observed_at":"2026-08-14T15:54:36.606572Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.590508Z","title":"Mott physics and spin fluctuations: A unified framework,","venue":null,"work_id":"befc3eab-937e-422c-a372-c63e17fc83d9","year":2015},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.618953Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:ff7f123f70716b994fb604961ae39c235da14ca64ba06da871dd595141e215ff","observation_id":"852d300e-8bf8-4f81-8dc8-6c877f9fbbe2","resolution":{"observed_at":"2026-08-14T15:54:36.595808Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.579739Z","title":"Mott physics and spin fluctuations: A functional viewpoint,","venue":null,"work_id":"9057c5d0-0789-4204-b474-9a129c900df2","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.622906Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:df7ff3a5fb37ea9398f455fd785db9a9d2d1b8f164fee506c999fb41407d5e6f","observation_id":"c0b11fa8-ebfa-4007-9519-84e399fd6294","resolution":{"observed_at":"2026-08-14T15:54:36.583735Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.567299Z","title":"Fierz convergence criterion: A controlled approach to strongly inter- acting systems with small embedded clusters,","venue":null,"work_id":"c1b61a7b-b327-425b-b52e-b877a0fc6816","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.626811Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:659dc9826f7e5f745a3d1b2375053854cf1da0ff48ff16a09acd281ddf123fd5","observation_id":"f8014e6f-3d2b-4a71-928e-d3a3b9d26167","resolution":{"observed_at":"2026-08-14T15:54:36.572357Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.556104Z","title":"Dynamical Cor- relations and Screened Exchange on the Experimental Bench: Spectral Properties of the Cobalt Pnictide BaCo 2As2,","venue":null,"work_id":"a5fe43df-052c-4556-930a-f3a2f6e11efa","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.630316Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:90f3641897c42080b8d3409bb17f894acae5db4fb018cffb7fd08d413645dfe4","observation_id":"29b812c7-bcdd-4008-9772-588990a5da27","resolution":{"observed_at":"2026-08-14T15:54:36.560071Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.542157Z","title":"Combined GW and dy- namical mean-field theory: Dynamical screening effects in tran- sition metal oxides,","venue":null,"work_id":"04f8ded4-9dba-4f31-9818-b2e9f0b29d43","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.634067Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:f01521d37df8a4fc7d4b5a3d37189cfbd0e2afbaad304966b1cbcd2257890674","observation_id":"92c00931-cd8c-4473-8707-a883fb522902","resolution":{"observed_at":"2026-08-14T15:54:36.546447Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.531531Z","title":"Comparing quasiparticleGW+DMFT and LDA+DMFT for the test bed material SrVO 3,","venue":null,"work_id":"596b77e1-93b8-4dc7-bafb-0fc20b561511","year":2013},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.638447Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:75e7372b4cd59f8721eb09786da1d7503e32ad06e4487dea88efb2635e022650","observation_id":"f63b718f-5730-46d0-b2d3-bd91ca550f98","resolution":{"observed_at":"2026-08-14T15:54:36.535182Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.520608Z","title":"Electronic structure of SrVO 3 within GW+DMFT,","venue":null,"work_id":"3fd0cab8-b075-4eaa-bbc2-5c262c49eb6c","year":2013},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.642329Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:041a2e445b98965cef83385c5eeed61a60063b5c6abde165f39dea7f957178b0","observation_id":"a69844a8-0771-4c0d-a831-1678767323a8","resolution":{"observed_at":"2026-08-14T15:54:36.524350Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.509752Z","title":"Tomczak, M","venue":null,"work_id":"fc1335b1-9a94-4522-86ea-a3a5bc486baf","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.646811Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:0d3bc21d3f69ccd2785fad86d38ddca95b725dbd84e990a405c41bb1955e7a90","observation_id":"e76002e2-e5bf-4b11-883b-c3d469e71e3f","resolution":{"observed_at":"2026-08-14T15:54:36.513641Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.498485Z","title":"Nonequilibrium dynami- cal mean-field theory and its applications,","venue":null,"work_id":"b9842d67-6165-4ebf-a9fa-f706839bdeaa","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.650734Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:c5e9d4c023e09b21ac08abd618273de5bfa85ed24faf01898488b0485ba31d89","observation_id":"37407699-4281-444e-93a6-1320d7e7c8d0","resolution":{"observed_at":"2026-08-14T15:54:36.502142Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.488202Z","title":"Nonequilibrium GW + EDMFT: Antiscreening and Inverted Populations from Nonlocal Corre- lations,","venue":null,"work_id":"37c14e09-754f-419d-a7d7-8dbc7f4b4170","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.654730Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:b5545f25f50b52d13e9f475a440a78d04a4d82c5002f6093649e71ec46d73b76","observation_id":"a21ab1bb-281f-4c0c-b353-0da93e10cdeb","resolution":{"observed_at":"2026-08-14T15:54:36.491899Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.476732Z","title":"On a method of calculating quantum dis- tribution functions,","venue":null,"work_id":"10a9e30c-a5ed-4b00-bd97-e0ad8eb13a9e","year":1957},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.658433Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d3051806a19369b09a8fd21b755cb65902463d1ad531e598c34ccc315e5647c2","observation_id":"82cdb148-fdd0-41cf-b2a0-b53c6c4adaa1","resolution":{"observed_at":"2026-08-14T15:54:36.481262Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.465703Z","title":"Calculation of partition functions,","venue":null,"work_id":"243668d5-e3b6-4ab7-bba4-19848c844445","year":1959},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.662186Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:16932245df333170f3bf6a9f9435939a5b638c8ccb6c0eab4aa496a8a5b1f5ad","observation_id":"fbb094fe-cfdc-4f10-a494-257e6ac55699","resolution":{"observed_at":"2026-08-14T15:54:36.470087Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.452793Z","title":"Continuous-time quantum Monte Carlo method for fermions,","venue":null,"work_id":"8802b112-1e06-426e-82e9-c0a2e11a6aa2","year":2005},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.666123Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:73ba91c06f0e1c2b81d245f28a2ce5edb06390ee50df9bae232b9e3f620782c8","observation_id":"267511c4-dbcf-4582-ab23-ccdbe83240a2","resolution":{"observed_at":"2026-08-14T15:54:36.456993Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.440327Z","title":"Continuous-time solver for quantum impurity models,","venue":null,"work_id":"0b52b1c7-ff9f-4410-8123-d3dc1b2ebff5","year":2006},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.670060Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:baeee037c18e47256063bd664d403e9af7c14e3501f457cfedd263bd810febf7","observation_id":"b61c16bf-d7c9-44de-928f-334668119732","resolution":{"observed_at":"2026-08-14T15:54:36.444640Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.429698Z","title":"Dynamical screening in correlated electron materials,","venue":null,"work_id":"c845015d-c5c3-450c-aca8-76da64580a4f","year":2010},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.673788Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:7e8c9c6435d3be7fed5608419c18194d27a5e8f100b113459e16c6ce2abf70e3","observation_id":"4b83acdd-d787-47b2-b227-cf4556048c24","resolution":{"observed_at":"2026-08-14T15:54:36.433353Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.419340Z","title":"Continuous-time monte carlo methods for quantum impurity models,","venue":null,"work_id":"87e4bcc2-e50b-44b2-a0b1-5fbf988970f8","year":2011},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.677637Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:b4038cdd73e7b0d82735de7c74ba736e07b792aa4061e10861a1bfec64da3f89","observation_id":"4aac2f2c-864c-4b11-ae25-8c6cdc349e32","resolution":{"observed_at":"2026-08-14T15:54:36.423280Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.408254Z","title":"Dual fermion approach to nonlocal correlations in the hubbard model,","venue":null,"work_id":"5d933e2a-dae5-4c2c-9dbd-e96af4c9c327","year":2008},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.681857Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:5ac346e9f6988686b8330644210eb7248531603a21385573d1201c80dd8fecc1","observation_id":"e5b2d4d9-314b-48f5-8598-001db1033f8a","resolution":{"observed_at":"2026-08-14T15:54:36.412076Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.397753Z","title":"Dual boson approach to collective excitations in correlated fermionic systems,","venue":null,"work_id":"e6712137-21dd-4583-9641-5b51c303089e","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.685731Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:648e3f6475bc543000f88cdf18b46108830604073a35f431aa94532bf383c703","observation_id":"59de66e5-550b-4990-a06c-b7090e0eb886","resolution":{"observed_at":"2026-08-14T15:54:36.401439Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.386583Z","title":"Self-consistent dual boson approach to single-particle and collective excitations in correlated systems,","venue":null,"work_id":"5cf77957-fa45-4b25-91ee-77fd0f83aba7","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.689207Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:117f3907f643ebb96362ef850752e4af034438cb789198fd2944c8bec3d3d005","observation_id":"1e049e5b-b170-46d3-adab-a86a23872b36","resolution":{"observed_at":"2026-08-14T15:54:36.390629Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.374616Z","title":"From local to nonlocal correla- tions: The Dual Boson perspective,","venue":null,"work_id":"fd3b7f67-5282-4e31-896e-dc76abada7ac","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.692704Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:3f7ca924a8a41f69e788fd9baa5f691eb316137305f28ecfd3152742b67d2a6e","observation_id":"359fa5b7-6e9a-4649-b700-1d5507c5ddda","resolution":{"observed_at":"2026-08-14T15:54:36.378393Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.359284Z","title":"Di- agrammatic monte carlo approach for diagrammatic extensions of dynamical mean-field theory: Convergence analysis of the dual fermion technique,","venue":null,"work_id":"65e53c1d-840b-4cfd-a15c-0c95218ea65d","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.696280Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cf201dccd5ad3ceb758d60e2c91908f7bb33696d4df87e193812f82e6ecce173","observation_id":"d8ee91a7-d35c-47a4-a4b4-2202f43eaba5","resolution":{"observed_at":"2026-08-14T15:54:36.363348Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.344162Z","title":"Dia- grammatic Monte Carlo for dual fermions,","venue":null,"work_id":"4305d3d0-d99b-445c-befb-c8a4af073746","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.700096Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d02cca8ad594c17a545842209fd02d9fe2986e7dbdcfa8e43abd38835cdfe49b","observation_id":"c33d38ab-1478-4259-bdd4-0de6138efc70","resolution":{"observed_at":"2026-08-14T15:54:36.348634Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.332611Z","title":"Momentum-space cluster dual-fermion method,","venue":null,"work_id":"8c98bfbe-44a2-439c-9fee-a40cec9fb1ee","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.703734Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:143b31d62ccfc3f8576da6c3b6e05d79dbb0f1f108c33ceb37f8fec0b2e8d452","observation_id":"94fe3324-b819-4517-be68-1cb175cf61a8","resolution":{"observed_at":"2026-08-14T15:54:36.336338Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.321660Z","title":"Efficient perturbation theory for quantum lattice models,","venue":null,"work_id":"fb5dfe76-d8ed-488e-af25-f068b247c703","year":2009},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.707039Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cbfb2d0d740b977784a5fb8daed0e4f933ec1d2168f60e4b51b1f6e526f9228b","observation_id":"537f7c27-c2d9-4146-b430-65d9f2bb4383","resolution":{"observed_at":"2026-08-14T15:54:36.325695Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.308851Z","title":"Mul- titier self-consistent GW + EDMFT,","venue":null,"work_id":"feff8324-5c85-406b-ac67-5db1c671aed6","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.710491Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:7f19938b83d334417fc352a7a6677327777c00b779dce7ad2a7b0b00c05f1d65","observation_id":"4e851927-0ebf-413b-adb1-f8a9462517a5","resolution":{"observed_at":"2026-08-14T15:54:36.312871Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.297830Z","title":"Many- Body Effects in Iron Pnictides and Chalcogenides: Nonlocal Versus Dynamic Origin of Effective Masses,","venue":null,"work_id":"a73cdc7a-6623-44ed-9f80-2645aa58f18f","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.714329Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:69ec7c19a05ab81a51127deaa428a48b5c09f3d9f08ba2d92636cd442f14b3b5","observation_id":"82d9e9b0-00e9-4d61-9ae1-131ab1ec0ba7","resolution":{"observed_at":"2026-08-14T15:54:36.301912Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1906.11853","last_updated":"2020-10-23T13:46:24Z","snapshot_observed_at":"2026-08-14T16:10:47.273490Z","submitted_at":"2019-06-27T18:00:06Z","title":"Effect of non-local correlations on the electronic structure of LiFeAs","version":3},"cited_work":{"arxiv_id":"1906.11853","doi":null,"metadata_source":"pith","pith_arxiv_id":"1906.11853","snapshot_observed_at":"2026-08-14T15:54:35.905138Z","title":"Effect of non-local correlations on the electronic structure of LiFeAs","venue":"cond-mat.str-el","work_id":"b5bb9fbb-13ca-460d-bef2-ea928063404f","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.717826Z"},"links":{"cited_paper":"/paper/1906.11853","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:a7cd51333dca857bca54063245202072bfb03e97c7ff1ff4aeded20fc346aac2","observation_id":"00f56b97-79a0-4577-949f-046b22124a28","resolution":{"observed_at":"2026-08-14T15:54:35.908938Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.284720Z","title":"Generalized Hedin’s Equa- tions for Quantum Many-Body Systems with Spin-Dependent Interactions,","venue":null,"work_id":"65485d7d-37e6-490d-abea-4fffc2feb37f","year":2008},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.721329Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:c957e3a3050cb9635d48dc214350c414026917b3e13bfdbca205c1f88c722e62","observation_id":"a8249f4c-eea5-47a0-9372-2b5cdf7113bf","resolution":{"observed_at":"2026-08-14T15:54:36.289089Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.272524Z","title":"Self-energies in itinerant magnets: A focus on Fe and Ni,","venue":null,"work_id":"24bdf3db-1cff-46d1-b5f6-f95c68495943","year":2017},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.724148Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d2c8afc3ee6da38096df8813b54075060baafc159756806807a645e27a89a6ce","observation_id":"231fe348-53b9-4fe4-8e5f-6943b5d97b2c","resolution":{"observed_at":"2026-08-14T15:54:36.276809Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.259944Z","title":"Ab initio calculations of quasiparticle band structure in correlated systems: LDA ++ approach,","venue":null,"work_id":"d206eee9-ef38-48cf-bfaa-1a23062ccc73","year":1998},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.727028Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:54dc87841f9268cc68171e043fcd23be6dea550c6e21f8e9d6eb7fa1f0e654de","observation_id":"924bb1c8-238b-4fde-a5f4-a96a6691a4d1","resolution":{"observed_at":"2026-08-14T15:54:36.264121Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.246616Z","title":"E ffective action for strongly correlated fermions from functional integrals,","venue":null,"work_id":"8ed4b92f-60cc-425f-a84d-a87791806bfa","year":1990},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.730008Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cf07decf29466046098fc2988d567d6a53bbdcf0e8e4fd7acae41607ae5215fc","observation_id":"e168cee9-0354-4018-82a3-0d6bb8dc9204","resolution":{"observed_at":"2026-08-14T15:54:36.250407Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.235063Z","title":"E fficient parametrization of the vertex function, Ω scheme, and the t, t ′ hubbard model at van hove filling,","venue":null,"work_id":"d4dcd04e-eb0c-4170-b327-debb1f331fb2","year":2009},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.732941Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:243718342c3f2d2452ab9a843f932805ac31979866dadb50dba5b17e50ae7365","observation_id":"eb3130dd-9479-446e-a528-04ea190ad942","resolution":{"observed_at":"2026-08-14T15:54:36.239253Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.223529Z","title":"Four-point vertex in the Hubbard model and partial bosonization,","venue":null,"work_id":"c25a592a-4a17-40cf-83dd-9552dfca7366","year":2010},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.736216Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:443f0e83d9aca946d1b1fbc84499e68f2eba7b2f7eae6a4eb54e7a5d952a7f63","observation_id":"ecacac84-9a40-415a-b001-f700ad91ed92","resolution":{"observed_at":"2026-08-14T15:54:36.227576Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.209832Z","title":"Fluctuation Di- agnostics of the Electron Self-Energy: Origin of the Pseudogap Physics,","venue":null,"work_id":"f7c0c408-8e23-456e-9009-b7b997056902","year":2015},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.740496Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:ae3e67fff192c26f0d49e1c6ca48acc77ed69bb5937864cf89e3893f0843df0f","observation_id":"d757ebfd-94db-4785-8d88-f2c1f74dd65b","resolution":{"observed_at":"2026-08-14T15:54:36.215271Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.196052Z","title":"E ffective Heisenberg Model and Exchange Interaction for Strongly Correlated Systems,","venue":null,"work_id":"49e77e68-48dd-43cc-b083-649153cbf24d","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.743935Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:3fc4f2c083e2306c9924af8e833429d1993f2fc0bb551b52dfdb57a77ecc1332","observation_id":"5ff73e35-6fa4-4415-839a-8f348d33f69b","resolution":{"observed_at":"2026-08-14T15:54:36.200622Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.183357Z","title":"Effective Ising model for correlated systems with charge ordering,","venue":null,"work_id":"2f0d7202-acbf-4772-bd86-6397206010f2","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.747650Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:90dc064aa252768211d1c535c4a6eb3090a2a9c24b6a7b2ceb65c627d1f1e712","observation_id":"f56622c1-aba9-4e6c-8646-56008ba17b8f","resolution":{"observed_at":"2026-08-14T15:54:36.187374Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.172455Z","title":"Local electronic cor- relation at the two-particle level,","venue":null,"work_id":"78b5bd8e-29db-4710-872c-462b8625d687","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.752017Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:a456090e7a0755d3279bf89b67b2da1737d99d10a039a616423e0664a4652215","observation_id":"b7d27456-6cc2-496e-9722-7cac59ad26ed","resolution":{"observed_at":"2026-08-14T15:54:36.175870Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1610.06520","last_updated":"2020-07-02T19:48:19Z","snapshot_observed_at":"2026-08-14T21:34:17.796383Z","submitted_at":"2016-10-20T17:54:13Z","title":"High-frequency asymptotics of the vertex function: diagrammatic parametrization and algorithmic implementation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.06520","snapshot_observed_at":"2026-08-14T15:54:35.756038Z","title":"High-frequency asymptotics of the vertex function: diagrammatic parametriza- tion and algorithmic implementation,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.756038Z"},"links":{"cited_paper":"/paper/1610.06520","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:c2fd058824addc9f38993d353b6b0c073d33e0bbfc98b570777a3f943446cdd3","observation_id":"9a8360a0-393a-424d-91f2-6b3ca43bb292","resolution":{"observed_at":"2026-08-14T15:54:35.756038Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.161403Z","title":"Renormalization-group ac- celeration of self-consistent field solutions: Two-dimensional hubbard model,","venue":null,"work_id":"fb55a1fc-57af-4942-9406-3e3e17735e4c","year":1994},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.760147Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:db7e6924923c4e1aeb0667336e8b2d0a96362433a6552d9d25dae6b2ebf0f3ff","observation_id":"736190ab-1f6b-49c6-8459-881a85436082","resolution":{"observed_at":"2026-08-14T15:54:36.165196Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.03581","last_updated":"2020-01-10T11:15:07Z","snapshot_observed_at":"2026-08-16T05:53:50.912221Z","submitted_at":"2019-07-08T13:03:14Z","title":"Single-boson exchange decomposition of the vertex function","version":2},"cited_work":{"arxiv_id":"1907.03581","doi":null,"metadata_source":"pith","pith_arxiv_id":"1907.03581","snapshot_observed_at":"2026-08-14T15:54:35.876159Z","title":"Single-boson exchange decomposition of the vertex function","venue":"cond-mat.str-el","work_id":"1077d29d-594b-4254-83c5-a74bb9594d02","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.763944Z"},"links":{"cited_paper":"/paper/1907.03581","citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:4b9e3ee43a2fd377d21572dd0d147061b3eb0d74c9d40b545cd7f0dee3c75fd0","observation_id":"cf3d2c7a-1443-406c-b59e-50fe887b2ae0","resolution":{"observed_at":"2026-08-14T15:54:35.882153Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.150654Z","title":"E ffi- cient implementation of the continuous-time hybridization ex- pansion quantum impurity solver,","venue":null,"work_id":"f7d17991-e706-4ee6-a2b5-28b444899f7d","year":2013},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.767951Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:44b7f934a5e0ff3990c4f59c4920e8d096a9875c5d4185a3362ed0b0112c804f","observation_id":"688fcaef-b375-4787-9e99-ba6203ed7fd8","resolution":{"observed_at":"2026-08-14T15:54:36.154602Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.139479Z","title":"Self-energy and vertex functions from hybridization-expansion continuous-time quantum monte carlo for impurity models with retarded interaction,","venue":null,"work_id":"e1d32c49-bbab-49fa-b153-2e85f990538d","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.771677Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:8d2ac72220ab16ad4ad5f9ca8c9984f187e5689ad891e3b0f869f77106b0026c","observation_id":"9c22979b-2dbd-468a-b96b-e6d674c80d87","resolution":{"observed_at":"2026-08-14T15:54:36.143441Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.128740Z","title":"The ALPS project release 2.0: open source software for strongly correlated systems,","venue":null,"work_id":"1bc169f8-4f25-4fb2-9eed-dcc0edf86797","year":2011},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.775478Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:54de602318cb57be7f1456c5325c323377a48574476d230f7f63531f599aeaad","observation_id":"4576d5e8-e052-46ea-87bc-d7d0e588c620","resolution":{"observed_at":"2026-08-14T15:54:36.132258Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.116920Z","title":"Be- yond extended dynamical mean-field theory: Dual boson ap- proach to the two-dimensional extended Hubbard model,","venue":null,"work_id":"bc1e2bc9-940a-44ea-9fb0-63f151bcf246","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.779374Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:3ce4cdf63ab841482f853d27a86eecc7841ff14731de2eaf45154051115c19a9","observation_id":"cc062e18-0e24-4915-970a-3e571e176b07","resolution":{"observed_at":"2026-08-14T15:54:36.120874Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.105430Z","title":"Cluster Dynamical Mean Field Theory of the Mott Transition,","venue":null,"work_id":"051befce-879c-46d1-b5e4-4bafbac963e1","year":2008},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.783349Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:3142f22bc4a96e57afdebb943afeb9b61381c4b711eda80c1f286e796a76063c","observation_id":"8f3bdf80-65f3-4114-a2cb-fe80937c4221","resolution":{"observed_at":"2026-08-14T15:54:36.110363Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.094022Z","title":"Second-order dual fermion approach to the Mott transition in the two-dimensional Hubbard model,","venue":null,"work_id":"2f5f27b6-3564-465d-a28e-96f025eaac77","year":2018},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.787136Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:98436bd2cd90c16b6449b244a0ad91f345b3f91699391647d5124bf6dc3fb565","observation_id":"d3879a87-47fa-4a44-970f-3a1fd8ed6fc5","resolution":{"observed_at":"2026-08-14T15:54:36.098241Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.083725Z","title":"Functional renormal- ization group approach to correlated fermion systems,","venue":null,"work_id":"fb852216-49ae-41b3-a061-8ffa98d0378b","year":2012},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.790865Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:74e97f0ccc2df940471b3bf7bdb13092e82bb32c5e98ca32a3cb99d4d6bd763b","observation_id":"8cc785e4-634c-4b05-8dd9-2585099fd5cf","resolution":{"observed_at":"2026-08-14T15:54:36.087575Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.071397Z","title":"Functional renormal- ization group for multi-orbital fermi surface instabilities,","venue":null,"work_id":"b2b03e0c-cba7-4a52-8733-0295d8336e96","year":2013},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.794961Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:80ef0d538966aeece3d931229a7ca096508065ecd9e149bdd099ba3d10a6bf25","observation_id":"e8d6ca31-4d2c-42d0-83f7-0981d863be5f","resolution":{"observed_at":"2026-08-14T15:54:36.075680Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.059450Z","title":"From infinite to two dimensions through the functional renormalization group,","venue":null,"work_id":"c54e70a4-b277-424e-9f5a-e14f5d4a2df0","year":2014},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.798927Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:e9f0f8c4fc0632ad9dad886a030db99147c2cf0d17754e150003ae952c12eeb7","observation_id":"930ff89c-f818-4bfa-8d8e-e75e455658f3","resolution":{"observed_at":"2026-08-14T15:54:36.063581Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.047053Z","title":"Correlated starting points for the functional renormal- ization group,","venue":null,"work_id":"f9188229-203e-475a-84a1-7ef394485711","year":2015},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.803083Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:cdc9c1367b1fe4257134e4fac592dd61c70859edd4ed78d588fc3c41d245a70b","observation_id":"8f3b859f-f836-4157-840f-4a5d1fc1994a","resolution":{"observed_at":"2026-08-14T15:54:36.050527Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.033856Z","title":"Extended dynamical mean field the- ory combined with the two-particle irreducible functional renormalization-group approach as a tool to study strongly cor- related systems,","venue":null,"work_id":"cabae0ea-6ff6-4f2f-8751-45afc759b525","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.806731Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:de0a55e80b732aeee9dec890b0925c915cf74183e3551a7735cc42b1a548bb21","observation_id":"4bdc7644-d8f5-4cad-8f35-5dff8960e2c5","resolution":{"observed_at":"2026-08-14T15:54:36.038442Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.021980Z","title":"Multiloop functional renormalization group for the two- dimensional Hubbard model: Loop convergence of the re- sponse functions,","venue":null,"work_id":"0d90e3b1-9448-4b4d-a7a7-2171b9f09cf6","year":2019},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.811012Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:c756a07ee9df0d2172a73f70d21a742b7fba0d00b046a311e9a72247a20d98ea","observation_id":"562ffd26-f39b-4422-9ff2-0f649a7c8c93","resolution":{"observed_at":"2026-08-14T15:54:36.026058Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:36.011320Z","title":"E ffects of van hove singularities on magnetism and superconductivity in the t− t ′ hubbard model: A parquet approach,","venue":null,"work_id":"4dc8a4d8-1023-4a72-9944-05b41710e502","year":2001},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.815609Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:46e2b4dc30fff309711d2d7bdda1b7947a1e5acf40fa879ec424f7c165313fba","observation_id":"a7d89642-18ae-4a05-a3e6-7a8ff60bfa6a","resolution":{"observed_at":"2026-08-14T15:54:36.014984Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.999782Z","title":"Dynamical vertex approximation in its parquet implementation: Applica- 13 tion to hubbard nanorings,","venue":null,"work_id":"45340cb1-6191-4e9d-8b70-e8e6584cbb59","year":2015},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.819852Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:345678a018a90686e99f443844f1af0ca378c68dffeb882593ab97ad48402bc8","observation_id":"879c9c95-f411-48b5-9dc5-bd8f3f5dbf01","resolution":{"observed_at":"2026-08-14T15:54:36.004145Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.987886Z","title":"E fficient implementation of the parquet equa- tions: Role of the reducible vertex function and its kernel ap- proximation,","venue":null,"work_id":"20cee5fa-a114-4c76-b9b5-f2c546691229","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.824078Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:6902ad7289f3824bd5c72f19400b97e9e1f9db731b4f21612a73b4b534ab34c6","observation_id":"43d8fe20-6427-447d-8b2d-c1f46215fc37","resolution":{"observed_at":"2026-08-14T15:54:35.992013Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.975482Z","title":"Parquet decomposi- tion calculations of the electronic self-energy,","venue":null,"work_id":"cacdecef-82dc-40c0-ba48-7c18d39c9b1d","year":2016},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.828045Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:d493dee57de8222e7bcc624b0425ac0a7792feb75bcc941f6c5e121d6d7b3276","observation_id":"399e1be4-03f3-463d-a47c-a4bebc65071a","resolution":{"observed_at":"2026-08-14T15:54:35.979775Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:54:35.963980Z","title":"Conserving approximations for strongly fluctuating electron systems. I. Formalism and cal- culational approach,","venue":null,"work_id":"e71c11c3-3673-4516-8e19-06f16bdc6c5a","year":1989},"citing_paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-14T15:54:35.833002Z"},"links":{"citing_paper":"/paper/1908.00536"},"observation_digest":"sha256:f31ae6a5685b635138c9cff090e53fd4a4d11c5558ce14ac8e6b4f309c432574","observation_id":"0b9cf7cd-7fdd-494d-8744-3b0bb0805b9b","resolution":{"observed_at":"2026-08-14T15:54:35.968220Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"1908.00536","last_updated":"2019-11-06T12:13:11Z","latest_version":2,"primary_category":"cond-mat.str-el","snapshot_observed_at":"2026-08-16T05:46:21.129235Z","submitted_at":"2019-08-01T17:49:11Z","title":"Consistent partial bosonization of the extended Hubbard model"},"reference_resolution":{"displayed":98,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":19,"verified_exact":5,"verified_fuzzy":74},"total_outbound_references":98},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"thesis":"As of 16 August 2026, this Paper Citation Record lists 98 of 98 outbound references and 1 inbound Pith citation observation for arXiv:1908.00536."}