{"as_of":"2026-08-20T10:56:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:3a7e39a6e10239468669d67b67ee2c0748de4429fd5e9bf2e43a9856c4a2a17f","coverage":[{"denominator":179,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T04:01:16.838783Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-20T06:33:59.587034+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":"2026-08-07T19:53:03.218141Z","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":"2026-08-07T19:53:04.162413Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"cited_work":{"arxiv_id":"2602.06298","doi":null,"metadata_source":"pith","pith_arxiv_id":"2602.06298","snapshot_observed_at":"2026-08-07T19:53:04.162413Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","venue":"cond-mat.str-el","work_id":"0e0f2030-f05c-4d13-be09-30e6e8ebee78","year":2026},"citing_paper":{"arxiv_id":"2608.05988","last_updated":"2026-08-06T13:02:44Z","snapshot_observed_at":"2026-08-19T09:40:48.329720Z","submitted_at":"2026-08-06T13:02:44Z","title":"Resilient strange metal at an unconventional quantum critical point in $d=2$","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-07T19:53:03.218141Z"},"links":{"cited_paper":"/paper/2602.06298","citing_paper":"/paper/2608.05988"},"observation_digest":"sha256:8998c636c397174df159359498ee621b0dd4c526fc7dc50147eaa290a1da87d3","observation_id":"2a524ec2-8f2d-417b-8467-d92d6a04ebe5","resolution":{"observed_at":"2026-08-07T19:53:04.167574Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2602.06298/citation-record","integrity":"/paper/2602.06298/integrity","json":"/paper/2602.06298/citation-record.json","paper":"/paper/2602.06298"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T04:01:04.367341Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:04.367341Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a6081c2b793f7d5bba41111e72d932597fe91329314ec1180a5731d66f1826aa","observation_id":"aa483c29-3c7a-4fe0-9ebc-391a02395561","resolution":{"observed_at":"2026-08-03T04:01:04.367341Z","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":"2026-08-03T04:01:04.493771Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:04.493771Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:9490440c852b92b2b3d3f470041fca574e9162e934767740b7db023fc5faa79a","observation_id":"b42817f2-3b3e-4b10-ade6-b6cf07f5fc6e","resolution":{"observed_at":"2026-08-03T04:01:04.493771Z","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":"2026-08-03T04:01:04.636884Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:04.636884Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:d9d9057fd2a47cae81121788ed2c9270b07f8760e76b03cddf29de6df5af77a4","observation_id":"de852179-286c-4628-8bc1-94d58d60605a","resolution":{"observed_at":"2026-08-03T04:01:04.636884Z","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":"2026-08-03T04:01:04.888210Z","title":"Proust and L","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:04.888210Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:dfddb00109c5c038c37cd4a298c4fdb3435a40dfda2c1d4361d1585865a03555","observation_id":"e36adb47-a5a5-4b90-bc8d-2afbb38a1aa6","resolution":{"observed_at":"2026-08-03T04:01:04.888210Z","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":"2026-08-03T04:01:05.007959Z","title":"Kampf and J","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.007959Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:1309565b843c29857e0db313d019dc77b6c194097bf40a7971789b66e9cddd8e","observation_id":"834099f6-8beb-492a-85fa-4408eaf1e36d","resolution":{"observed_at":"2026-08-03T04:01:05.007959Z","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":"2026-08-03T04:01:05.157186Z","title":null,"venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.157186Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8c586f4f4d1d6702a37b75e66b755f52fab72c099c7c18db90600df4b71393f9","observation_id":"1769f1cd-0193-45d8-91a5-608849caad76","resolution":{"observed_at":"2026-08-03T04:01:05.157186Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"cond-mat/9702188","last_updated":"1997-12-11T14:57:58Z","snapshot_observed_at":"2026-07-07T02:47:29.826814Z","submitted_at":"1997-02-20T22:09:21Z","title":"Non-perturbative many-body approach to the Hubbard model and single-particle pseudogap","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"cond-mat/9702188","snapshot_observed_at":"2026-08-03T04:01:05.264745Z","title":null,"venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.264745Z"},"links":{"cited_paper":"/paper/cond-mat/9702188","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:c4e5ab7031532418df7e491eae4a2b88f343f89356a443a7d774a73abacaa0f8","observation_id":"a82741e2-268e-47f4-9918-18bef4e315da","resolution":{"observed_at":"2026-08-03T04:01:05.264745Z","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":"2026-08-03T04:01:05.367393Z","title":"Varma, Non-fermi-liquid states and pairing instability of a general model of copper oxide metals, Physical Review B55, 14554 (1997)","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.367393Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:056ddcc6d536889c83ddeaa1e111c936f2c903c79f043f0626d4c10ae179baba","observation_id":"25cb9ca3-9f6b-4647-8e5e-fe55f4c654b5","resolution":{"observed_at":"2026-08-03T04:01:05.367393Z","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":"2026-08-03T04:01:05.464570Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.464570Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:b0a8d99cd333fe271d5bd54b9a3443847d9e2e6d0d1742caceea506887c286fb","observation_id":"4c3b8d23-0372-4cd8-b952-062fa00f6e49","resolution":{"observed_at":"2026-08-03T04:01:05.464570Z","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":"2026-08-03T04:01:05.581893Z","title":"Franz and A","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.581893Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8256fe9141854fb9661442a7fc597dbbedc30b761992478d6de8576b6713bbf9","observation_id":"77c3a8cd-6504-44b7-9bc1-e4d2bb7c36d5","resolution":{"observed_at":"2026-08-03T04:01:05.581893Z","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":"2026-08-03T04:01:05.640967Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.640967Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:19a5d0843f7648f823a99578d664054220d90a4688a68d8f7901f7fa25293045","observation_id":"3babe4f4-0a0c-4823-9306-4ab1a0215631","resolution":{"observed_at":"2026-08-03T04:01:05.640967Z","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":"2026-08-03T04:01:05.713966Z","title":"Schmalian, D","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.713966Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:adfd1e5a3b6a6e4a03a890da4043d1233c8f7236c897ac607b5f9e56c03f4455","observation_id":"022e0ab5-9996-42d3-9300-c04822e8498e","resolution":{"observed_at":"2026-08-03T04:01:05.713966Z","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":"2026-08-03T04:01:05.768371Z","title":"Sénéchal and A.-M","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.768371Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:72b3191b36e25d8e9e547487a7522f3c0318584415bbe50ef690ad23d7cfb488","observation_id":"ea580f6b-d5d9-49e1-a2be-10e9e128622c","resolution":{"observed_at":"2026-08-03T04:01:05.768371Z","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":"2026-08-03T04:01:05.810242Z","title":"Kyung, S","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.810242Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:ffe2893db38aae6b952101d44a4142778f32681719dac894a6dddaded39c0549","observation_id":"078ce083-5526-4146-bafc-df0b3f67c2cd","resolution":{"observed_at":"2026-08-03T04:01:05.810242Z","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":"2026-08-03T04:01:05.881461Z","title":"Ferrero, P","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:05.881461Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:d3cdfccd0d2e5e6f5a526a91253f5a9e00a3eb6bab21c4fe11e0a69852a5f9d8","observation_id":"25b4bc8e-7656-4691-bdd7-aa719c811408","resolution":{"observed_at":"2026-08-03T04:01:05.881461Z","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":"2026-08-03T04:01:06.008405Z","title":"Liebsch and N.-H","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.008405Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:747168a911ac418a8197b618c05ae3580046762cd51c0c6e52d507970ed521dd","observation_id":"7bf2b10c-5b21-4c9e-aa6e-7ec89455a535","resolution":{"observed_at":"2026-08-03T04:01:06.008405Z","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":"2026-08-03T04:01:06.096461Z","title":"Sordi, K","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.096461Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:bca6caafbef4a4e9cf1dd400566f79dfc8b9eb8d351b0d8c39fb92a21f5bc3cf","observation_id":"4c760899-c651-46c0-9017-fed759c97a4d","resolution":{"observed_at":"2026-08-03T04:01:06.096461Z","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":"2026-08-03T04:01:06.266247Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.266247Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:e0791d51176d8ab8c5e7b6f0c3ab527123b73da36411b301a55f354a4f2d4a6c","observation_id":"84c3cf9d-d35e-497a-85e6-08f6e99d2bc9","resolution":{"observed_at":"2026-08-03T04:01:06.266247Z","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":"2026-08-03T04:01:06.417554Z","title":"Sordi, P","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.417554Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:b3169dbd3f04f1d797abddf71720e33e219d34590f14a2d24e64a0be651ff70f","observation_id":"70745f15-da90-4329-9e9e-95a27cb46c8b","resolution":{"observed_at":"2026-08-03T04:01:06.417554Z","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":"2026-08-03T04:01:06.497257Z","title":"Gull and A","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.497257Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:65d27493493c82d83c64cda6ce15f98f466be1b35ff886852e514618023300d3","observation_id":"dffe619f-10ea-4908-8a33-0e0bb66b1722","resolution":{"observed_at":"2026-08-03T04:01:06.497257Z","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":"2026-08-03T04:01:06.741286Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.741286Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:5a2215a887dd74b681e86e20e022a5b35da109988cf5bd03916fafa15d622d46","observation_id":"3e499cb2-b8aa-4834-b475-23e8f9ffe716","resolution":{"observed_at":"2026-08-03T04:01:06.741286Z","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":"2026-08-03T04:01:06.801777Z","title":"Pépin, V","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.801777Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:694f033d9b307ec7cb8392cb96023e204894bfcf8fde3577090cf0b1bbd540cc","observation_id":"891eb87f-c9f7-4e0f-98be-818c398483ec","resolution":{"observed_at":"2026-08-03T04:01:06.801777Z","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":"2026-08-03T04:01:06.871986Z","title":"Atkinson, A","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.871986Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a2139c3c3bf8388f1b694b39b044aaa70067a4dd6fc7c4ed8900ebf0d26938ef","observation_id":"c3a3208a-1107-4f6d-b4fc-49a4df1d6564","resolution":{"observed_at":"2026-08-03T04:01:06.871986Z","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":"2026-08-03T04:01:06.926915Z","title":"Chowdhury and S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.926915Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a333baa0385dabe03005b7cf1799b413043cb4c0a5b71ea918dc9e9fd6d02ea6","observation_id":"42b4f032-6e09-4a03-8729-181bc2d68f67","resolution":{"observed_at":"2026-08-03T04:01:06.926915Z","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":"2026-08-03T04:01:06.997193Z","title":"Fratino, P","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:06.997193Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a15d112013367429960a7be752f713e3e83a91ead1b36615a08b60c57603334b","observation_id":"86ef38fb-834b-43ef-b52c-934ba4623516","resolution":{"observed_at":"2026-08-03T04:01:06.997193Z","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":"2026-08-03T04:01:07.052436Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.052436Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8e4486ca66eed0bb4b29e602d3cdc8ffe3c272394deb53550e07cbaebad69f5b","observation_id":"44c3015b-bb17-4292-8601-d9869cdb9f5b","resolution":{"observed_at":"2026-08-03T04:01:07.052436Z","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":"2026-08-03T04:01:07.131363Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.131363Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:d1cd8779de1fb78d09256b2092358f823a4fa5a64ec931fbf356808564ed90e2","observation_id":"9de33051-d29e-4472-8313-ff4e201c41f6","resolution":{"observed_at":"2026-08-03T04:01:07.131363Z","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":"2026-08-03T04:01:07.186934Z","title":"Wu, S.-S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.186934Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:6c016de3a9ee5d7e7b276669be4384d151c7a2cdf3dcd2af219db43b84040355","observation_id":"6e5520b8-4b16-4f02-9874-48f1d5c0efc9","resolution":{"observed_at":"2026-08-03T04:01:07.186934Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.06572","last_updated":"2021-09-14T10:40:05Z","snapshot_observed_at":"2026-08-16T17:56:45.530360Z","submitted_at":"2021-09-14T10:40:05Z","title":"Doping-driven pseudogap-metal-to-metal transition in correlated electron systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.06572","snapshot_observed_at":"2026-08-03T04:01:07.252822Z","title":"Fratino, S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.252822Z"},"links":{"cited_paper":"/paper/2109.06572","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:0a333ade502018cb5855aaf693e5949100929f07be2de1fdcf5a4c103c345e96","observation_id":"84e745fc-c62f-48ef-a3d4-60b11e9fec89","resolution":{"observed_at":"2026-08-03T04:01:07.252822Z","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":"2026-08-03T04:01:07.331632Z","title":"Gauvin-Ndiaye, P.-A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.331632Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:07aaec6d68875be10b35edce7dd0064ca4921c9bf81acb8b266708a76c1f1bea","observation_id":"998cb710-e1fb-4713-8048-eba0ef05806a","resolution":{"observed_at":"2026-08-03T04:01:07.331632Z","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":"2026-08-03T04:01:07.543506Z","title":"Wang and Y","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.543506Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:ed4e143513de772497c0f810c780066c0278a999a09c53217660d8e111352f2d","observation_id":"0f8d37dc-b907-4863-87ed-9b608b7cccdb","resolution":{"observed_at":"2026-08-03T04:01:07.543506Z","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":"2026-08-03T04:01:07.689889Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.689889Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:15608699b83a03323b0a237359c302e0bf9f3aed50051f7de598d73009fd02df","observation_id":"8fce5d83-f15c-4537-83a1-b00c80ce5392","resolution":{"observed_at":"2026-08-03T04:01:07.689889Z","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":"2026-08-03T04:01:07.826575Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.826575Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:9c933b257ce429522a9fad08c71c381b4d0f1e8f29b530714e20e54ca4cb53ca","observation_id":"21763489-a37f-422a-9df6-297941bd3eeb","resolution":{"observed_at":"2026-08-03T04:01:07.826575Z","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":"2026-08-03T04:01:07.990211Z","title":"Ye and A","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:07.990211Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:6ac9785e5b70749d210868ae60dabf5b93dbf6be382864b7e3ee106300457edf","observation_id":"c3637f81-0eba-42d8-85e8-8b6e1315a823","resolution":{"observed_at":"2026-08-03T04:01:07.990211Z","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":"2026-08-03T04:01:08.142336Z","title":"Sakai, Nonperturbative calculations for spectroscopic prop- erties of cuprate high-temperature superconductors, Journal of the Physical Society of Japan92, 092001 (2023)","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.142336Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:2c6408f232db1d4919fef3a1e91ad16340873ee0f2f20efee9a7d81f1ccfacfc","observation_id":"9b3e046d-ccdc-4582-841d-66fde62cf689","resolution":{"observed_at":"2026-08-03T04:01:08.142336Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.11727","last_updated":"2025-08-25T00:27:06Z","snapshot_observed_at":"2026-08-17T18:54:11.131093Z","submitted_at":"2025-05-16T22:21:16Z","title":"Pseudogap in electron-doped cuprates: thermal precursor to magnetism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.11727","snapshot_observed_at":"2026-08-03T04:01:08.258876Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.258876Z"},"links":{"cited_paper":"/paper/2505.11727","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:550d3077daf8bf74d52f273507bc5eb0039ad39d12cdfb187db368256b691bb1","observation_id":"b807c408-afc7-46d6-9077-55d399c0d859","resolution":{"observed_at":"2026-08-03T04:01:08.258876Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.20164","last_updated":"2026-04-29T18:37:36Z","snapshot_observed_at":"2026-08-15T03:30:45.131843Z","submitted_at":"2025-08-27T18:00:01Z","title":"Fractionalized Fermi liquids and the cuprate phase diagram","version":7},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.20164","snapshot_observed_at":"2026-08-03T04:01:08.421787Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.421787Z"},"links":{"cited_paper":"/paper/2508.20164","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:944bff766edaaf92f6f88ec03e4740620f6364c7c749668099e29571cf51d452","observation_id":"e9acf3bb-3dfa-4eb7-869a-1a369c286481","resolution":{"observed_at":"2026-08-03T04:01:08.421787Z","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":"2026-08-03T04:01:08.541153Z","title":"Zhang and S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.541153Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a2795b5d9cfbd614340bccf97743cc7b458b78c75fc7b39f1679ec81a5bca09e","observation_id":"70eb217b-14c3-4d45-9878-ed829baa91bf","resolution":{"observed_at":"2026-08-03T04:01:08.541153Z","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":"2026-08-03T04:01:08.649518Z","title":"Meixner, H","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.649518Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:f2a028c8c973c3e152628fd2d530db9756806d17f5813415d1758d5ab345795d","observation_id":"7ded0dbe-61f4-4a2a-a11a-c3eac1a88c20","resolution":{"observed_at":"2026-08-03T04:01:08.649518Z","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":"2026-08-03T04:01:08.754095Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.754095Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:31d164c7ed3e8fbd5b0dd132530cc2e7722c4311dfd9975327d6004fa56c58fd","observation_id":"1a8c19c2-234f-412b-ae36-2a32a7ac0915","resolution":{"observed_at":"2026-08-03T04:01:08.754095Z","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":"2026-08-03T04:01:08.845893Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.845893Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:95a52636f0e618b12e7046d3d8c59617725cbb86e438e97b56e122ddc654c64f","observation_id":"86f4ed7f-452b-408d-9844-4621887a77e0","resolution":{"observed_at":"2026-08-03T04:01:08.845893Z","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":"2026-08-03T04:01:08.913625Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:08.913625Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:263d9f14ae1e4d900aa9b114eb998df2812f90fe52e5e2b941b28fe4fcb05f80","observation_id":"273cb5da-2546-412b-96d2-7c4e551a70e0","resolution":{"observed_at":"2026-08-03T04:01:08.913625Z","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":"2026-08-03T04:01:09.029452Z","title":"Chalopin, P","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.029452Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:7e0b25869a453d94f37d50568900dc91378766931ed06ec8e041e7755f6c5d77","observation_id":"0236476d-b85b-4152-be44-f0d9f2351e68","resolution":{"observed_at":"2026-08-03T04:01:09.029452Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.04743","last_updated":"2018-02-13T17:08:15Z","snapshot_observed_at":"2026-08-14T19:46:17.101156Z","submitted_at":"2018-02-13T17:08:15Z","title":"Direct sampling of the self-energy with Connected Determinant Monte Carlo","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.04743","snapshot_observed_at":"2026-08-03T04:01:09.105771Z","title":"Rossi, Direct sampling of the self-energy with connected determinant monte carlo (2018), arXiv:1802.04743 [cond- mat.str-el]","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.105771Z"},"links":{"cited_paper":"/paper/1802.04743","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:9d18261e544c62e97e9787631a63996889e58dac877c03a65bf5e337360488b4","observation_id":"63f4f15e-2ba8-482d-b372-02f694e25b78","resolution":{"observed_at":"2026-08-03T04:01:09.105771Z","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":"2026-08-03T04:01:09.213523Z","title":"Šimkovic and E","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.213523Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:464c5785715dc022b78256b804cadd748aa704e16c3e1144a0ca8df97217feee","observation_id":"a404b770-7a46-4d1c-be09-e96ebb5df75c","resolution":{"observed_at":"2026-08-03T04:01:09.213523Z","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":"2026-08-03T04:01:09.329736Z","title":"Šimkovic, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.329736Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:f74f3a415c66ea2742542916effac8a3e5dc23c91db9192ccafdb1429db62458","observation_id":"468ba50e-a754-4503-a5bd-dd4812dba797","resolution":{"observed_at":"2026-08-03T04:01:09.329736Z","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":"2026-08-03T04:01:09.460905Z","title":"Šimkovic IV , J","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.460905Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:1867052a4f421002d61f08ffb0eceaf5bc49da74d602fad0983a55e1da8517b3","observation_id":"735e2888-fba1-49cc-afc2-77ecc8ed4bc5","resolution":{"observed_at":"2026-08-03T04:01:09.460905Z","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":"2026-08-03T04:01:09.575253Z","title":"Schäfer, N","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.575253Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:2e29ea14d499b4b3c27e67aac6541b5b1f4840a0781a31b8a313f2789163e269","observation_id":"b74bbf25-58fa-467a-8172-efbfe70ae6cf","resolution":{"observed_at":"2026-08-03T04:01:09.575253Z","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":"2026-08-03T04:01:09.700120Z","title":"Moukouri, S","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.700120Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:4e645218aa4dc6db4e9c620360c89c7cd8adf5bab2cfb3d59033fea65d3f0ff7","observation_id":"84e06514-7b61-49c7-9727-f9509896ba34","resolution":{"observed_at":"2026-08-03T04:01:09.700120Z","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":"2026-08-03T04:01:09.848098Z","title":"Schäfer, F","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.848098Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:7b1f67f11bd497702cbbda8b7a9f6bfe9effcd8f64bedb58fa246ca5f1f08122","observation_id":"79065b6d-7a3a-45a6-ac00-acf2b9775080","resolution":{"observed_at":"2026-08-03T04:01:09.848098Z","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":"2026-08-03T04:01:09.971677Z","title":"Sinha and A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:09.971677Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:2ff82fb9d942fefde2daedd1bcc7f95656d42ebbe6d1bc2a66934a287ffc37c6","observation_id":"adc10f27-8beb-423d-b62f-f3788850f0a0","resolution":{"observed_at":"2026-08-03T04:01:09.971677Z","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":"2026-08-03T04:01:10.121938Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.121938Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:7b91b2c44434521d7d0a55ec9f52e8af4d634fee62cf4cf14c8d6428bd13b756","observation_id":"90981378-58c9-4a2b-bb19-38e8c8ec0200","resolution":{"observed_at":"2026-08-03T04:01:10.121938Z","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":"2026-08-03T04:01:10.254729Z","title":"Gauvin-Ndiaye, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.254729Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:82f63c0690d171af83f5195a2c7e3c4c247be7c9576cd1e47dde7874723d1118","observation_id":"0e2489f7-1b3b-484f-8a0b-47435c693927","resolution":{"observed_at":"2026-08-03T04:01:10.254729Z","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":"2026-08-03T04:01:10.397765Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.397765Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:69d6e44f51018b4b4bf5065743b8a6c95bd90993e9bbf402900a8f6c3f86affb","observation_id":"754dfe9a-8c64-493b-965e-4a95bd0cb1ca","resolution":{"observed_at":"2026-08-03T04:01:10.397765Z","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":"2026-08-03T04:01:10.516832Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.516832Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:f06b9c6f316e0ffcc425bedd0009a8ecbe88addedba0c041089cc6b93ff85cab","observation_id":"e342f3f8-5509-4b07-b827-99804c0233c4","resolution":{"observed_at":"2026-08-03T04:01:10.516832Z","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":"2026-08-03T04:01:10.652508Z","title":"Vilk, Criteria and analytical results for the pseudogap at the Van Hove point in two dimensions, Physical Review B108, 235110 (2023)","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.652508Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:dc511473c9c19682fbeb603c17844395c795f03fb5c636b8d1f17794500c1a85","observation_id":"d5167efa-06e8-47c0-8752-720d25978c47","resolution":{"observed_at":"2026-08-03T04:01:10.652508Z","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":"2026-08-03T04:01:10.783635Z","title":"Sordi, K","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.783635Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:24e1f8fb384d07650dc5af7cf9f4fe45fb012ba0cd55ea4d837e44f4ba2a1017","observation_id":"c48667fc-7a96-499b-bf5d-73bb5fd2aa95","resolution":{"observed_at":"2026-08-03T04:01:10.783635Z","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":"2026-08-03T04:01:10.958368Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:10.958368Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:e5a6ff373c6bca9b37ff5068ebce4a2ff68e5ba119504cfd8c601fb5073cca86","observation_id":"6df6079c-e30d-49a6-80c3-db6c2f0e7688","resolution":{"observed_at":"2026-08-03T04:01:10.958368Z","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":"2026-08-03T04:01:11.125621Z","title":"Fradkin, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.125621Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:21ef0d5ae1ea2460013d40b52da2b0f238c8e8a6382f00a15a350c2b713cf8c9","observation_id":"afc6bbf9-40e0-4eab-83ae-1e946ca40186","resolution":{"observed_at":"2026-08-03T04:01:11.125621Z","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":"2026-08-03T04:01:11.180372Z","title":"Šimkovic, R","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.180372Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:72d826e513d7e55658ef0df8cf52599e86e3462926521fb97532aa8c38cb85e4","observation_id":"6b8bbcee-75e7-40b0-b3b2-f6039cf3ccf1","resolution":{"observed_at":"2026-08-03T04:01:11.180372Z","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":"2026-08-03T04:01:11.280116Z","title":"Xiao, Y .-Y","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.280116Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:6d480fa08734ee0215d530a97df67d015fb67fb9e567d9523f602eb762cf0a43","observation_id":"2b9f18c4-39bc-4ee3-b55a-d54c11d56d6c","resolution":{"observed_at":"2026-08-03T04:01:11.280116Z","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":"2026-08-03T04:01:11.419188Z","title":"Zheng, C.-M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.419188Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:dd700f27f796a31997a180e34d5799eed8688e33c24ca44163097d73122eed79","observation_id":"5e44b20f-4117-4463-a0c3-fb01ae39f333","resolution":{"observed_at":"2026-08-03T04:01:11.419188Z","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":"2026-08-03T04:01:11.534765Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.534765Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:5d755eaa308172290dc45df4deab775bb7a2c231d830afd742e5754a7f380311","observation_id":"b88b96f0-dda7-4da3-a087-cb0aab9f5667","resolution":{"observed_at":"2026-08-03T04:01:11.534765Z","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":"2026-08-03T04:01:11.781216Z","title":"Mushkaev, F","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.781216Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:35b261a4fcbdac9b8304c5c53efdc10a506f2b6c85e34dfb503c1cb018421458","observation_id":"d214b47a-8539-4e3d-b8b0-d9adec92c776","resolution":{"observed_at":"2026-08-03T04:01:11.781216Z","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":"2026-08-03T04:01:11.931846Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:11.931846Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:d648b8d8aa42bb744a038aaf32229a0fbaeb6100c221579cd8d2882eadca39ac","observation_id":"db3ca960-759c-4320-9d2c-ccce6ddd01f8","resolution":{"observed_at":"2026-08-03T04:01:11.931846Z","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":"2026-08-03T04:01:12.078167Z","title":"Vilk, Hierarchy of pseudogap crossovers and their evolution with coupling strength in the two-dimensional hubbard model (2025), unpublished manuscript","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.078167Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:ce40f6455fcb3b9b166f92f208c18509d4626a74fc16a7861b9d37642b0e54a0","observation_id":"361fa31a-f67e-4b68-a601-3d715a6f2590","resolution":{"observed_at":"2026-08-03T04:01:12.078167Z","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":"2026-08-03T04:01:12.290768Z","title":null,"venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.290768Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:bd859bb43d81399465898b5a7aedf942c9d1183fa896c250bb7615bd947bbcca","observation_id":"a5594606-0be1-43ea-ab90-83847dd7d484","resolution":{"observed_at":"2026-08-03T04:01:12.290768Z","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":"2026-08-03T04:01:12.500354Z","title":null,"venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.500354Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:24565efcb51853e66d1614f4409267659e15346a86681f2829cd88569bcd8fa2","observation_id":"b9e76a05-437e-4ed4-abcf-c8a0baa14528","resolution":{"observed_at":"2026-08-03T04:01:12.500354Z","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":"2026-08-03T04:01:12.630186Z","title":null,"venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.630186Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:b71a31fd08123c4691b4c2df5cb36a286c9ae33b10a211448359c5bc826f0eff","observation_id":"ad4dc6a4-79d5-4c8c-8a2a-47aa4579f196","resolution":{"observed_at":"2026-08-03T04:01:12.630186Z","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":"2026-08-03T04:01:12.828306Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.828306Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:9f50a21cd1e98138c810ad005bf8fe60d3c24f6fc99a5c8701da7695abf67462","observation_id":"18f22923-07da-4fd7-ba11-b5bae47c85ca","resolution":{"observed_at":"2026-08-03T04:01:12.828306Z","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":"2026-08-03T04:01:12.992227Z","title":"Hedayati and G","venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:12.992227Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:854910bef71524d585f90fdb6b798ddb1a31244ccc0e0d5989ef41ecfbbb20df","observation_id":"053269c6-b249-4c7b-8b53-ff433c48f766","resolution":{"observed_at":"2026-08-03T04:01:12.992227Z","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":"2026-08-03T04:01:13.172315Z","title":null,"venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.172315Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:17b40f62b33d935414fcf9846539a53f3b9124287eef90942f0d08822deba38e","observation_id":"c64b3e6c-7a9a-426f-9cab-446dc14efa05","resolution":{"observed_at":"2026-08-03T04:01:13.172315Z","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":"2026-08-03T04:01:13.342632Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.342632Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:6a38f5e4395336bcdf41e22fb19c2550067596635879d85099a6a9dfc791da63","observation_id":"2e12fc54-fd1d-4384-91e6-ecbd18e40852","resolution":{"observed_at":"2026-08-03T04:01:13.342632Z","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":"2026-08-03T04:01:13.464821Z","title":"Boyack, Q","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.464821Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:20d75d6c857b8c1001a5a1135e93b54330e70c59b22b212bdcfe2902baa5027e","observation_id":"5f52c970-5c60-4b0a-bf02-835c6231b27b","resolution":{"observed_at":"2026-08-03T04:01:13.464821Z","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":"2026-08-03T04:01:13.603509Z","title":"Shinaoka, J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.603509Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:4b6e863ff10cb0afcbe32ba486315ce82b3f57775a1e81e3f71a24a80ba8f612","observation_id":"9555a132-ae3a-4301-822d-b87532b3486b","resolution":{"observed_at":"2026-08-03T04:01:13.603509Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.11762","last_updated":"2022-06-23T15:01:00Z","snapshot_observed_at":"2026-08-16T16:50:51.260892Z","submitted_at":"2022-06-23T15:01:00Z","title":"sparse-ir: optimal compression and sparse sampling of many-body propagators","version":1},"cited_work":{"arxiv_id":"2206.11762","doi":"10.48550/arxiv.2206.11762","metadata_source":"pith","pith_arxiv_id":"2206.11762","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"sparse-ir: optimal compression and sparse sampling of many-body propagators","venue":"physics.comp-ph","work_id":"70145447-4a01-4a74-b410-5025cae91477","year":2022},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.771580Z"},"links":{"cited_paper":"/paper/2206.11762","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:6332fb4351c2e960b924f177467b06ec359da3033903830a88a89e662f6482aa","observation_id":"fc48f5ec-1fbf-4f71-add6-17d5395cb7f0","resolution":{"observed_at":"2026-08-03T04:03:19.185646Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+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":"2026-08-03T04:01:13.905129Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:13.905129Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:f08cf3adf0b779abf02b7eca8710f1744bebc2adb02a10ea480b751ac2ff660a","observation_id":"5e4ddf7c-283b-4386-a1e2-ad485fb9b064","resolution":{"observed_at":"2026-08-03T04:01:13.905129Z","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":"2026-08-03T04:01:14.079516Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.079516Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:7a6c4f38ecb45671359ee3e39f60461392ea16576070cabf3ded40cafe9716e5","observation_id":"95b6cc52-c35e-46a2-b506-f2b98ef71e86","resolution":{"observed_at":"2026-08-03T04:01:14.079516Z","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":"2026-08-03T04:01:14.204115Z","title":null,"venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.204115Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:98c5e9ee79e55dae75825f96d604a78c72d9abe7203d56738966ee90f3a6c0fa","observation_id":"e45f2bce-b6f5-4a82-b3d1-caa30a7570a9","resolution":{"observed_at":"2026-08-03T04:01:14.204115Z","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":"2026-08-03T04:01:14.324971Z","title":"Vilk, Shadow features and shadow bands in the paramag- netic state of cuprate superconductors, Physical Review B55, 3870 (1997)","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.324971Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:0c0147c27707401317244049633fb0151a90968389b4d9d0383dfdd570951c87","observation_id":"971e5b07-eae7-4564-ab3f-db66173f64bc","resolution":{"observed_at":"2026-08-03T04:01:14.324971Z","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":"2026-08-03T04:01:14.470247Z","title":"Maier, M","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.470247Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:2f703e1007e363b6f6aa40f3b7f969c21f4e9128b43b97238f539ff062c0fe81","observation_id":"80a12f23-f110-4240-a19d-e479781558fc","resolution":{"observed_at":"2026-08-03T04:01:14.470247Z","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":"2026-08-03T04:01:14.581017Z","title":"Kotliar, S","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.581017Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:863bbcab20ff35dc477877207ed2971dd2bc5e856af3b6f7af06427b6713ba61","observation_id":"b72cd8cd-ada0-4cb1-8cf4-62783137153b","resolution":{"observed_at":"2026-08-03T04:01:14.581017Z","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":"2026-08-03T04:01:14.709183Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.709183Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:0f8f64f34adf2efa6bf81437ef6a8024741165ae1fe1b2dc8463fe6bb1b0c87d","observation_id":"dd183e92-af01-4ed9-a65b-3deccb09fd9a","resolution":{"observed_at":"2026-08-03T04:01:14.709183Z","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":"2026-08-03T04:01:14.846393Z","title":"Potthoff, Cluster extensions of dynamical meanfield the- ory, Chap","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.846393Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:7b81270fe0fdc34fce15160d4954b4c57ae98390e4ffabd51f9648f3b1686ac3","observation_id":"30b77579-4b17-406f-bc0c-967f8609b487","resolution":{"observed_at":"2026-08-03T04:01:14.846393Z","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":"2026-08-03T04:01:14.978360Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:14.978360Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:e939e30aa684f26e9fc015ac15693849eff69b4075e07a120f68e8f5d0b6ba19","observation_id":"5a9923ba-af41-4dfc-89b9-44b4371c819d","resolution":{"observed_at":"2026-08-03T04:01:14.978360Z","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":"2026-08-03T04:01:15.071377Z","title":"Downey, O","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.071377Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8d9c9179b04e4fbe5d551cc9daed98df30ad9637936b1f4ccaa4c8bdf186edda","observation_id":"874557e1-f73e-4afd-9d5f-dc88c3920329","resolution":{"observed_at":"2026-08-03T04:01:15.071377Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.02302","last_updated":"2020-04-05T20:08:00Z","snapshot_observed_at":"2026-08-02T15:27:33.865180Z","submitted_at":"2020-04-05T20:08:00Z","title":"Mott transition and high-temperature crossovers at half-filling","version":1},"cited_work":{"arxiv_id":"2004.02302","doi":"10.48550/arxiv.2004.02302","metadata_source":"pith","pith_arxiv_id":"2004.02302","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","title":"Mott transition and high-temperature crossovers at half-filling","venue":"cond-mat.str-el","work_id":"30b9f3c2-bc8d-40ec-bcd3-ac2c7dd7b833","year":2020},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.212328Z"},"links":{"cited_paper":"/paper/2004.02302","citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:a4b502204bcb507f74729b9bd457e642cf3eb50b8bba6a98bd2258a1404b5847","observation_id":"bbf95296-63ca-4fa2-8d11-4b537f2895fc","resolution":{"observed_at":"2026-08-03T04:03:18.964637Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+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":"2026-08-03T04:01:15.357189Z","title":"Fratino, P","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.357189Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:f5bd73f443252fe40bfa2f61da66c7b4052dc0c13c089f17403730ba082f8474","observation_id":"866ac0b5-2d11-45db-9d8e-0b3a81c3b92d","resolution":{"observed_at":"2026-08-03T04:01:15.357189Z","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":"2026-08-03T04:01:15.499473Z","title":null,"venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.499473Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:556d19e5002c7979fb7fd805a86950804560bffa9a01ac7f7bba8695f591e140","observation_id":"cd6dffcb-0d6a-44f2-b1bb-fd1133e1305e","resolution":{"observed_at":"2026-08-03T04:01:15.499473Z","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":"2026-08-03T04:01:15.677947Z","title":"Biroli and G","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.677947Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:3749c48eebcd1e3631e338c340aca0ddc2ed4327337365c26974e7fbb2394f2d","observation_id":"fa7552f8-cc77-47e1-996a-90aef6ff6655","resolution":{"observed_at":"2026-08-03T04:01:15.677947Z","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":"2026-08-03T04:01:15.783026Z","title":"Jarrell, T","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.783026Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:12e6cd709837281a4117b92b1d3b3a06e47dd2f871a3aa457f605f558f4d69a6","observation_id":"b3b937e5-018b-4226-8bf6-2ef7442ca276","resolution":{"observed_at":"2026-08-03T04:01:15.783026Z","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":"2026-08-03T04:01:15.841336Z","title":"Georges, G","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.841336Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:208912971d2c41aae99f32a61be65dcbb8f75d9958617ca97d57645e55357c82","observation_id":"ee357b28-3b99-432e-b706-283a8c95ba70","resolution":{"observed_at":"2026-08-03T04:01:15.841336Z","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":"2026-08-03T04:01:15.904955Z","title":"Georges and G","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.904955Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:420fbb71dbd6b3db47ce912d87bfed1d820d7d7c75d83c723e1a5778a91c88f9","observation_id":"4b7d2ee1-b75c-4b91-bfdc-bfdedca851cc","resolution":{"observed_at":"2026-08-03T04:01:15.904955Z","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":"2026-08-03T04:01:15.962189Z","title":"Jarrell, Hubbard model in infinite dimensions: A quantum monte carlo study, Phys","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:15.962189Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:5d8fbdda35241d9d37b42a54bfb2a962e5baeaae268041714511852765b2218e","observation_id":"d5c4a044-8da2-4ef3-b197-9fd177d520b1","resolution":{"observed_at":"2026-08-03T04:01:15.962189Z","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":"2026-08-03T04:01:16.069941Z","title":"Huscroft, M","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.069941Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8fb672b479a758c263658a6efc9fa2d391b8ec3c776dcd149bf1f81a64918f22","observation_id":"170a69d8-08df-4094-b3c1-3f6e616b4842","resolution":{"observed_at":"2026-08-03T04:01:16.069941Z","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":"2026-08-03T04:01:16.240541Z","title":"Macridin, M","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.240541Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:8cf610eedfe7f7950588570cc7cd0d7902afcbc88f0536bd03443f74bb8e665e","observation_id":"9499785b-3181-45a8-9ab3-b6eedd53e441","resolution":{"observed_at":"2026-08-03T04:01:16.240541Z","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":"2026-08-03T04:01:16.410498Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.410498Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:1e6bb93caa152d05ab0b303445f87bd95728e01d1a522e6508104ed4f96a4504","observation_id":"f7dd5542-ffa9-4ebe-9c1b-b45ca2b79701","resolution":{"observed_at":"2026-08-03T04:01:16.410498Z","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":"2026-08-03T04:01:16.548016Z","title":"Sakai, Y","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.548016Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:d8dfeee8c8fab381f88f50d9d607e5eee90daac3ab4d11e7e5cbeb9abd75124f","observation_id":"7a891b1e-5eea-4ee7-af61-a83e48482e52","resolution":{"observed_at":"2026-08-03T04:01:16.548016Z","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":"2026-08-03T04:01:16.707582Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":101,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.707582Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:bc18adb0d77318d695d3694019fb13e4c64b25a00b304c97fa6a01aa056b6081","observation_id":"7064720b-49c9-4bd8-a736-fa9346b59c6e","resolution":{"observed_at":"2026-08-03T04:01:16.707582Z","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":"2026-08-03T04:01:16.838783Z","title":"Sordi, P","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model","version":3},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-08-03T04:01:16.838783Z"},"links":{"citing_paper":"/paper/2602.06298"},"observation_digest":"sha256:235bbd3a6429fc8c31ca6e39d9df3c7ffe6a7bcc9b63f697e30a05d49ff95045","observation_id":"f0572f06-1b5d-4f4c-9fff-66928254152d","resolution":{"observed_at":"2026-08-03T04:01:16.838783Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2602.06298","last_updated":"2026-07-21T13:08:35Z","latest_version":3,"primary_category":"cond-mat.str-el","snapshot_observed_at":"2026-08-14T23:11:35.369356Z","submitted_at":"2026-02-06T01:44:51Z","title":"Pseudogap, Fermi liquid, Van Hove singularity and maxima of the compressibility and of the Knight shift as a function of doping in the two-dimensional Hubbard model"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":98,"verified_exact":2,"verified_fuzzy":0},"total_outbound_references":179},"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":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"thesis":"As of 20 August 2026, this Paper Citation Record lists 100 of 179 outbound references and 1 inbound Pith citation observation for arXiv:2602.06298."}