{"as_of":"2026-08-11T14:29:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:2bc5fa51b265e2d7610650c544f694f42ad88c098c4e92fb71641f273d4d8621","coverage":[{"denominator":30,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":30,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T21:57:12.321005Z","state":"measured"},{"denominator":32,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":32,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-01T08:02:16.081022Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-15T10:15:26.976218Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"cited_work":{"arxiv_id":"2501.03509","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.03509","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Kotov,QCD thermal transition with overlap fermions, in42nd International Symposium on Lattice Field TheoryLattice 2025 talk slides","venue":null,"work_id":"b9c92e90-6a3b-4fee-8dba-4c3d7ec90759","year":2025},"citing_paper":{"arxiv_id":"2603.16230","last_updated":"2026-05-09T07:27:53Z","snapshot_observed_at":"2026-08-06T12:12:20.772277Z","submitted_at":"2026-03-17T08:10:35Z","title":"Lattice QCD at finite temperature and density","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-05-15T10:13:05.645478Z"},"links":{"cited_paper":"/paper/2501.03509","citing_paper":"/paper/2603.16230"},"observation_digest":"sha256:648b6d1586986b4d9f8f1ecdcc36763d747befaa92d290ef519dc6b6c1c5341c","observation_id":"c96368d0-db5c-4b49-ab18-b7ecc2e9cc54","resolution":{"observed_at":"2026-05-15T10:15:26.978443Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.03509","snapshot_observed_at":"2026-08-01T08:02:16.081022Z","title":"Goswami, Y","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21346","last_updated":"2026-07-23T14:13:47Z","snapshot_observed_at":"2026-08-08T21:19:46.063929Z","submitted_at":"2026-07-23T14:13:47Z","title":"Perturbative quantum electrodynamics with generalized domain wall fermions","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-01T08:02:16.081022Z"},"links":{"cited_paper":"/paper/2501.03509","citing_paper":"/paper/2607.21346"},"observation_digest":"sha256:dcd0fc2a2b94d2e0175ce85e4684d34dbfa803912a29c2e9e5cbf04da3cf8b45","observation_id":"92ca7e90-0720-43a8-8e68-8fad00335b44","resolution":{"observed_at":"2026-08-01T08:02:16.081022Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2501.03509/citation-record","integrity":"/paper/2501.03509/integrity","json":"/paper/2501.03509/citation-record.json","paper":"/paper/2501.03509"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0611014","last_updated":"2006-11-10T16:05:34Z","snapshot_observed_at":"2026-07-07T03:43:38.563500Z","submitted_at":"2006-11-10T16:05:34Z","title":"The order of the quantum chromodynamics transition predicted by the standard model of particle physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0611014","snapshot_observed_at":"2026-08-10T21:57:12.172521Z","title":"Aoki et al.,The Order of the quantum chromodynamics transition predicted by the standard model of particle physics,Nature443(2006) 675 [hep-lat/0611014]","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.172521Z"},"links":{"cited_paper":"/paper/hep-lat/0611014","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:29f70377469440715b7a2efa71f61bed90acf0cd2fd2b7c07d8b9392d860b710","observation_id":"18e9d30b-4c6d-4b50-a149-77acd0c28dd1","resolution":{"observed_at":"2026-08-10T21:57:12.172521Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0402115","last_updated":"2006-03-27T16:31:55Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2006-03-27T16:31:55Z","title":"QCD phase diagram and the critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0402115","snapshot_observed_at":"2026-08-10T21:57:12.178007Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.178007Z"},"links":{"cited_paper":"/paper/hep-ph/0402115","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:81047d6d30522eb2dfaa88755bc42888f0269bfa6ce5f351340a025ee817495e","observation_id":"23b7543c-67ee-4055-b972-690495b1c66c","resolution":{"observed_at":"2026-08-10T21:57:12.178007Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.5214","last_updated":"2014-11-05T00:04:30Z","snapshot_observed_at":"2026-07-06T02:50:29.201528Z","submitted_at":"2012-06-22T17:27:27Z","title":"The M\\\"obius Domain Wall Fermion Algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.5214","snapshot_observed_at":"2026-08-10T21:57:12.188249Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.188249Z"},"links":{"cited_paper":"/paper/1206.5214","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:87e81edcfa47f20ad0fd6228307f08e52d2f89778e41e4f79dbacc13c87c99f8","observation_id":"9b06f3f4-3764-4eeb-a334-170c9d0b2f1a","resolution":{"observed_at":"2026-08-10T21:57:12.188249Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.6941","last_updated":"2013-11-27T11:39:15Z","snapshot_observed_at":"2026-07-06T03:29:20.089806Z","submitted_at":"2013-11-27T11:39:15Z","title":"Large-scale simulations with chiral symmetry","version":1},"cited_work":{"arxiv_id":"1311.6941","doi":null,"metadata_source":"pith","pith_arxiv_id":"1311.6941","snapshot_observed_at":"2026-08-10T21:57:12.751151Z","title":"Large-scale simulations with chiral symmetry","venue":"hep-lat","work_id":"c7152388-8c0a-4428-957e-6ad4a705b762","year":2013},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.193642Z"},"links":{"cited_paper":"/paper/1311.6941","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:c7360118f50f136ab923c23360005dfbdd7d615653bae5325ca240b95ddadf5b","observation_id":"9dcc781a-36e5-402e-aae5-d04dcc87069c","resolution":{"observed_at":"2026-08-10T21:57:12.755969Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+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":"2026-08-10T21:57:12.199091Z","title":"Aoki et al.,2+1 flavor fine lattice simulation at finite temperature with domain-wall fermions, PoSLATTICE2021(2022) 609 [2112.11771]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.199091Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:4b238f6938f7bc8c2c1a6045b066618b3118f712ccbeeb53e768dfabae8d1e86","observation_id":"fbabda1d-dada-4a6b-9e35-5f543a8f3d1c","resolution":{"observed_at":"2026-08-10T21:57:12.199091Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.05884","last_updated":"2023-03-10T12:29:14Z","snapshot_observed_at":"2026-08-07T22:18:25.954642Z","submitted_at":"2023-03-10T12:29:14Z","title":"Thermodynamics with M\\\"obius domain wall fermions near physical point II","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.05884","snapshot_observed_at":"2026-08-10T21:57:12.204079Z","title":"Aoki et al.,Thermodynamics with Möbius domain wall fermions near physical point II, PoSLATTICE2022(2023) 176 [2303.05884]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.204079Z"},"links":{"cited_paper":"/paper/2303.05884","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:a79ca6ae784a04b464e81a664aba21a6039f37ebbba6ed8b7f3b3180e4387ba5","observation_id":"5d71b817-44b7-4a04-b5b7-3c1853666857","resolution":{"observed_at":"2026-08-10T21:57:12.204079Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1104.1627","last_updated":"2011-04-08T19:16:19Z","snapshot_observed_at":"2026-07-06T02:26:03.723768Z","submitted_at":"2011-04-08T19:16:19Z","title":"On the sign of kurtosis near the QCD critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.1627","snapshot_observed_at":"2026-08-10T21:57:12.209659Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.209659Z"},"links":{"cited_paper":"/paper/1104.1627","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:2ad476c3bb72b5209f0d7f8f1341eda16838b0fceb9cb19660b62f7d00d12c4b","observation_id":"50919d66-d3d8-44fa-8310-3d6ed99f896d","resolution":{"observed_at":"2026-08-10T21:57:12.209659Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.4630","last_updated":"2007-09-28T15:15:20Z","snapshot_observed_at":"2026-07-06T01:29:48.187342Z","submitted_at":"2007-09-28T15:15:20Z","title":"Domain-wall and overlap fermions at nonzero quark chemical potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.4630","snapshot_observed_at":"2026-08-10T21:57:12.214545Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.214545Z"},"links":{"cited_paper":"/paper/0709.4630","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:f2b8127e0c79a024004226e83b7275a19d2df2d781dc407dcf31f664d004d4b2","observation_id":"04803b97-c29d-4af5-989d-f4fa5e2aba96","resolution":{"observed_at":"2026-08-10T21:57:12.214545Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T21:57:12.881444Z","title":"8 (2+1)-Flavor QCD with MDW Fermions Jishnu Goswami","venue":null,"work_id":"7ff554ca-741a-4b35-a362-383909946054","year":2024},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.219252Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:0b2db3e51e07b548ba9f75bc878fc5e20665699117261ed8263ecf61f08b1c92","observation_id":"d5a0a9cd-9d9d-400a-994a-4391d8d4f91a","resolution":{"observed_at":"2026-08-10T21:57:12.886283Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T21:57:12.866648Z","title":"Hashimoto et al.,Residual mass in five-dimensional fermion formulations,PoS LATTICE2013(2014) 431","venue":null,"work_id":"3d0a2e01-c1d6-4366-b07b-55216d0b2f1a","year":2014},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.223808Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:948710e489fccca9610c093fb7e258c129b951748f026e55dc9a23d30c45fe95","observation_id":"6f535547-41b1-4f6b-87ac-d920ef541085","resolution":{"observed_at":"2026-08-10T21:57:12.871465Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2203.04938","last_updated":"2023-01-01T21:33:18Z","snapshot_observed_at":"2026-07-06T12:46:08.838773Z","submitted_at":"2022-03-09T18:38:02Z","title":"Form factors of $B\\to\\pi\\ell\\nu$ and a determination of $|V_{ub}|$ with M\\\"{o}bius domain-wall-fermions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.04938","snapshot_observed_at":"2026-08-10T21:57:12.228548Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.228548Z"},"links":{"cited_paper":"/paper/2203.04938","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:877cbaf4fec0fb4667454d6cee3149a45353990c8fb5c8bd0cf0d1e0ef49fdd4","observation_id":"27a90beb-69d5-4653-a1f0-3efc4cc1185f","resolution":{"observed_at":"2026-08-10T21:57:12.228548Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0305183","last_updated":"2003-09-29T13:31:15Z","snapshot_observed_at":"2026-08-02T20:00:40.688779Z","submitted_at":"2003-05-16T15:28:33Z","title":"The pressure of QCD at finite temperatures and chemical potentials","version":3},"cited_work":{"arxiv_id":"hep-ph/0305183","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0305183","snapshot_observed_at":"2026-08-10T21:57:12.581377Z","title":"The pressure of QCD at finite temperatures and chemical potentials","venue":"hep-ph","work_id":"b70067ad-6184-49f8-80bc-79633a51e79c","year":2003},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.233780Z"},"links":{"cited_paper":"/paper/hep-ph/0305183","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:4e65f2713c31e3699d82b47134fa207fa48be5de6cbeacdb815c4b3317da36a6","observation_id":"8fa4259b-f7ca-4b90-941d-c7b02ad2e249","resolution":{"observed_at":"2026-08-10T21:57:12.586514Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1307.8098","last_updated":"2013-12-23T20:53:56Z","snapshot_observed_at":"2026-07-06T03:19:33.641064Z","submitted_at":"2013-07-30T19:37:07Z","title":"Equation of State of hot and dense QCD: Resummed perturbation theory confronts lattice data","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.8098","snapshot_observed_at":"2026-08-10T21:57:12.239058Z","title":"Mogliacci, J","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.239058Z"},"links":{"cited_paper":"/paper/1307.8098","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:4eaec3a452a2881820a884277e99f9e5a955ad6173b5733b29791b80ad241a50","observation_id":"30d301e4-95d9-4a19-b598-e1219f566bed","resolution":{"observed_at":"2026-08-10T21:57:12.239058Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.2317","last_updated":"2013-11-20T19:54:40Z","snapshot_observed_at":"2026-07-06T03:22:34.701857Z","submitted_at":"2013-09-09T20:35:05Z","title":"Quark number susceptibilities at high temperatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.2317","snapshot_observed_at":"2026-08-10T21:57:12.243955Z","title":"Bazavov, H","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.243955Z"},"links":{"cited_paper":"/paper/1309.2317","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:a1d7cb0add5c49e826266ea0a9d390177641d6eeb99ef2b5eeb54d2685246b37","observation_id":"65d71c91-3537-4863-b5a0-d0bbf019db3f","resolution":{"observed_at":"2026-08-10T21:57:12.243955Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.06637","last_updated":"2015-10-26T18:02:38Z","snapshot_observed_at":"2026-08-03T20:24:50.469036Z","submitted_at":"2015-07-23T19:57:40Z","title":"Diagonal and off-diagonal quark number susceptibilities at high temperatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.06637","snapshot_observed_at":"2026-08-10T21:57:12.249036Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.249036Z"},"links":{"cited_paper":"/paper/1507.06637","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:c0c69d423b3d5e84e49474494462ada180275432769622eda3638d8770eab4af","observation_id":"a87bfc17-7ba8-4ba0-8785-6b38139dda0f","resolution":{"observed_at":"2026-08-10T21:57:12.249036Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.04627","last_updated":"2015-07-16T15:58:55Z","snapshot_observed_at":"2026-08-10T15:28:09.145523Z","submitted_at":"2015-07-16T15:58:55Z","title":"Fluctuations and correlations in high temperature QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.04627","snapshot_observed_at":"2026-08-10T21:57:12.253779Z","title":"Bellwied, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.253779Z"},"links":{"cited_paper":"/paper/1507.04627","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:040f5a95a6d17f265cdea3198dd793bb16560db81581f50682417c7e3822274c","observation_id":"54ce167e-af39-4474-8763-56388786937b","resolution":{"observed_at":"2026-08-10T21:57:12.253779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.09184","last_updated":"2022-05-02T02:23:42Z","snapshot_observed_at":"2026-08-08T08:20:01.612629Z","submitted_at":"2022-02-18T13:26:59Z","title":"Taylor expansions and Pad\\'e approximants for cumulants of conserved charge fluctuations at non-vanishing chemical potentials","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.09184","snapshot_observed_at":"2026-08-10T21:57:12.258297Z","title":"Bollweg, J","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.258297Z"},"links":{"cited_paper":"/paper/2202.09184","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:3873dfd793c08a2edb553719c10486624cc14b460c8964b6cee8b014470e6c6e","observation_id":"eca2f64f-c389-4700-bd35-d92b88475cbc","resolution":{"observed_at":"2026-08-10T21:57:12.258297Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.4416","last_updated":"2011-12-19T17:35:58Z","snapshot_observed_at":"2026-08-10T07:35:20.151746Z","submitted_at":"2011-12-19T17:35:58Z","title":"Fluctuations of conserved charges at finite temperature from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.4416","snapshot_observed_at":"2026-08-10T21:57:12.263064Z","title":"Borsanyi, Z","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.263064Z"},"links":{"cited_paper":"/paper/1112.4416","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:5e96248fabab0850fc654700ce2422d809eea6af991473da1493a64478d71808","observation_id":"be64417c-7403-47a8-b3d9-f5ae0c8d0cee","resolution":{"observed_at":"2026-08-10T21:57:12.263064Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.1710","last_updated":"2012-03-08T15:44:29Z","snapshot_observed_at":"2026-07-06T02:37:09.138894Z","submitted_at":"2011-11-07T20:57:56Z","title":"The chiral and deconfinement aspects of the QCD transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.1710","snapshot_observed_at":"2026-08-10T21:57:12.267940Z","title":"Bazavov et al.,The chiral and deconfinement aspects of the QCD transition,Phys","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.267940Z"},"links":{"cited_paper":"/paper/1111.1710","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:cffc9ab519ca763a82067591969487a3d66f43ee7985db36d2a961750366f229","observation_id":"8b603a28-3efc-4363-b880-e43669bf2bfd","resolution":{"observed_at":"2026-08-10T21:57:12.267940Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.10011","last_updated":"2021-11-05T08:33:41Z","snapshot_observed_at":"2026-08-11T01:45:58.472063Z","submitted_at":"2021-07-21T11:12:27Z","title":"Second order cumulants of conserved charge fluctuations revisited I. Vanishing chemical potentials","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.10011","snapshot_observed_at":"2026-08-10T21:57:12.272928Z","title":"Bollweg, J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.272928Z"},"links":{"cited_paper":"/paper/2107.10011","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:69c31ba48b0fc5d7da5b700fbc4e695b079fc84625eb00728a073204847d74b8","observation_id":"177cac7e-f377-4a00-b11d-b5a437669d33","resolution":{"observed_at":"2026-08-10T21:57:12.272928Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.07510","last_updated":"2015-11-12T13:59:39Z","snapshot_observed_at":"2026-08-09T14:55:34.402433Z","submitted_at":"2015-07-27T18:21:17Z","title":"The QCD phase diagram from analytic continuation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.07510","snapshot_observed_at":"2026-08-10T21:57:12.277289Z","title":"Bellwied, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.277289Z"},"links":{"cited_paper":"/paper/1507.07510","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:0285f6932e93dfcd912d5a1def0168a850df025edc5533340eb7be03a2a3ca0d","observation_id":"93e0996f-953c-4213-8afc-1a017e6d47bd","resolution":{"observed_at":"2026-08-10T21:57:12.277289Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.1558","last_updated":"2014-08-26T15:25:16Z","snapshot_observed_at":"2026-08-07T03:01:33.730465Z","submitted_at":"2014-02-07T06:31:24Z","title":"Beam energy dependence of moments of the net-charge multiplicity distributions in Au+Au collisions at RHIC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.1558","snapshot_observed_at":"2026-08-10T21:57:12.281613Z","title":"113(2014)092301[ 1402.1558]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.281613Z"},"links":{"cited_paper":"/paper/1402.1558","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:6dc596b8b8768e5ece3a28f3810e09029484b6e14a0d4166dce622d7ded9a3de","observation_id":"31811a46-756d-4125-9db9-5826f5a15f1a","resolution":{"observed_at":"2026-08-10T21:57:12.281613Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.07834","last_updated":"2016-01-24T20:40:39Z","snapshot_observed_at":"2026-07-06T04:22:02.594728Z","submitted_at":"2015-06-25T17:53:27Z","title":"Measurement of higher cumulants of net-charge multiplicity distributions in Au$+$Au collisions at $\\sqrt{s_{_{NN}}}=7.7-200$ GeV","version":2},"cited_work":{"arxiv_id":"1506.07834","doi":null,"metadata_source":"pith","pith_arxiv_id":"1506.07834","snapshot_observed_at":"2026-08-10T21:57:12.404217Z","title":"Measurement of higher cumulants of net-charge multiplicity distributions in Au$+$Au collisions at $\\sqrt{s_{_{NN}}}=7.7-200$ GeV","venue":"nucl-ex","work_id":"3224635d-7f6c-4304-b648-7cfe1c9f2a78","year":2015},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.286943Z"},"links":{"cited_paper":"/paper/1506.07834","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:e7cf10f9d0b85a499f44522b6dee77e75ca4aa8f172614dc94d5a9676f889d3b","observation_id":"67b150a5-7a39-4a03-95ea-06b16138860c","resolution":{"observed_at":"2026-08-10T21:57:12.411449Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1512.03487","last_updated":"2015-12-10T23:51:19Z","snapshot_observed_at":"2026-08-06T17:01:06.540703Z","submitted_at":"2015-12-10T23:51:19Z","title":"Grid: A next generation data parallel C++ QCD library","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.03487","snapshot_observed_at":"2026-08-10T21:57:12.291791Z","title":"Boyle, A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.291791Z"},"links":{"cited_paper":"/paper/1512.03487","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:70781c0bdd73f0a4c78549c8ffb5e9eefa7cc22431a8049ba1164a44cb411920","observation_id":"9845d063-ad05-4839-8f33-344b4650fb07","resolution":{"observed_at":"2026-08-10T21:57:12.291791Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T21:57:12.851886Z","title":"Grid: Data parallel c++ mathematical object library","venue":null,"work_id":"217d6a4c-ac86-4b7f-b644-475a31f44ce1","year":null},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.296846Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:e8f23ffafd8740dacafff06ba9d9d86eca10353164574593f677167aa97c583f","observation_id":"1fb3b277-7a16-4468-aea7-87104d0cf5d5","resolution":{"observed_at":"2026-08-10T21:57:12.856873Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T21:57:12.836905Z","title":"Ueda et al.,Development of an object oriented lattice QCD code ’Bridge++’, J","venue":null,"work_id":"9f415f44-ee8d-467d-9051-3a188f2c032b","year":2014},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.301561Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:0261c61e200071c1be77db280c84da9441eeb9d90f8272e88e7a1deffd29f962","observation_id":"be1c0e02-848d-4290-bf21-0961545fdcdb","resolution":{"observed_at":"2026-08-10T21:57:12.841785Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2303.05883","last_updated":"2023-03-10T12:26:31Z","snapshot_observed_at":"2026-08-06T04:22:51.800052Z","submitted_at":"2023-03-10T12:26:31Z","title":"Bridge++ 2.0: Benchmark results on supercomputer Fugaku","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.05883","snapshot_observed_at":"2026-08-10T21:57:12.306485Z","title":"Aoyama et al.,Bridge++ 2.0: Benchmark results on supercomputer Fugaku,PoS LATTICE2022(2023) 284 [2303.05883]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.306485Z"},"links":{"cited_paper":"/paper/2303.05883","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:5155e7adbcd63349a2f9424fbd83ad4e07242cf6b6e6b77f3d9bfad5879646dd","observation_id":"0978f994-1562-473e-a34e-aeadaa95616b","resolution":{"observed_at":"2026-08-10T21:57:12.306485Z","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":"2026-08-10T21:57:12.311696Z","title":"Lattice qcd code bridge++","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.311696Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:cc2ed1c68e4258544775ec1567a79647decb96ca6df2ebde194d989defdd863b","observation_id":"6e9dc20d-522c-407f-bf0d-1c48e8789358","resolution":{"observed_at":"2026-08-10T21:57:12.311696Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.06652","last_updated":"2023-09-24T17:34:42Z","snapshot_observed_at":"2026-07-06T16:05:39.158819Z","submitted_at":"2023-08-12T23:07:43Z","title":"Streamlined data analysis in Python","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.06652","snapshot_observed_at":"2026-08-10T21:57:12.316180Z","title":"Altenkort, D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.316180Z"},"links":{"cited_paper":"/paper/2308.06652","citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:be9c48f308cb60a725d318e04c19e5a04aae6009e85b78382497eefb959ecbb9","observation_id":"a0f8d4c8-72dc-42e0-a6b6-5f8e26a0e51b","resolution":{"observed_at":"2026-08-10T21:57:12.316180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T21:57:12.812347Z","title":"Analysistoolbox","venue":null,"work_id":"db7a2565-4102-4a17-af8b-854d350dfc63","year":null},"citing_paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-10T21:57:12.321005Z"},"links":{"citing_paper":"/paper/2501.03509"},"observation_digest":"sha256:8ab720888c39e67bf7cd52c14e7ba0cc0657e4b1b2b43413d3ebe9374759419b","observation_id":"0f3c5d73-186f-4271-aac5-b33ddcfa93bd","resolution":{"observed_at":"2026-08-10T21:57:12.817043Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2501.03509","last_updated":"2025-01-07T03:59:35Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-10T23:54:30.599939Z","submitted_at":"2025-01-07T03:59:35Z","title":"Quark number susceptibility and conserved charge fluctuation for (2+1)-flavor QCD with M\\\"obius domain wall fermions"},"reference_resolution":{"displayed":30,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":22,"verified_exact":3,"verified_fuzzy":5},"total_outbound_references":30},"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":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 30 of 30 outbound references and 2 inbound Pith citation observations for arXiv:2501.03509."}