{"as_of":"2026-08-16T20:10:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:9d01ddb1117bce1e90a803a6bd3835a83292f2bd05c59dbe8795aaa72ff400f0","coverage":[{"denominator":14,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":14,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T10:58:04.939006Z","state":"measured"},{"denominator":14,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":14,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-16T06:30:59.297886+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1908.10116/citation-record","integrity":"/paper/1908.10116/integrity","json":"/paper/1908.10116/citation-record.json","paper":"/paper/1908.10116"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0610092","last_updated":"2006-10-15T16:20:44Z","snapshot_observed_at":"2026-08-15T11:00:10.095389Z","submitted_at":"2006-10-15T16:20:44Z","title":"Highly Improved Staggered Quarks on the Lattice, with Applications to Charm Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0610092","snapshot_observed_at":"2026-08-14T10:58:04.888826Z","title":"Follana et al","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.888826Z"},"links":{"cited_paper":"/paper/hep-lat/0610092","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:be54c2a40f68e8aec8d2ee946beab81a27e562944397999809e88e32e8713e37","observation_id":"f0354e85-99b7-4095-8ccf-6cba2cda9052","resolution":{"observed_at":"2026-08-14T10:58:04.888826Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.05552","last_updated":"2023-02-02T11:42:59Z","snapshot_observed_at":"2026-08-14T21:11:34.241979Z","submitted_at":"2017-03-16T10:39:26Z","title":"Nonperturbative comparison of clover and HISQ quarks in lattice QCD and the properties of the phi meson","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.05552","snapshot_observed_at":"2026-08-14T10:58:04.893276Z","title":"Chakraborty et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.893276Z"},"links":{"cited_paper":"/paper/1703.05552","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:f27235eb475b442984afc18039929850d5264f9e0625552d972f004267a2073e","observation_id":"33ed01d3-d894-41e6-b090-02930e904187","resolution":{"observed_at":"2026-08-14T10:58:04.893276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0901.2599","last_updated":"2010-04-22T22:15:43Z","snapshot_observed_at":"2026-08-15T05:57:06.832292Z","submitted_at":"2009-01-19T19:02:26Z","title":"Renormalization of quark bilinear operators in a momentum-subtraction scheme with a nonexceptional subtraction point","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0901.2599","snapshot_observed_at":"2026-08-14T10:58:04.897046Z","title":"Sturm, Y","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.897046Z"},"links":{"cited_paper":"/paper/0901.2599","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:abae7b5aeedd2086cfcdf89c50f74d791b111b59f28531e6a06147df79000a17","observation_id":"4ebb8628-92d4-4e9d-af79-bfd29de632e7","resolution":{"observed_at":"2026-08-14T10:58:04.897046Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.3881","last_updated":"2013-10-17T10:47:12Z","snapshot_observed_at":"2026-08-15T00:13:49.708925Z","submitted_at":"2013-06-17T14:55:38Z","title":"Non-perturbative Renormalization for Improved Staggered Bilinears","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.3881","snapshot_observed_at":"2026-08-14T10:58:04.901127Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.901127Z"},"links":{"cited_paper":"/paper/1306.3881","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:30e9a27981f838a59c5b42e68860e7591b02acdb88ce8b91322b6ed9cc7f9b57","observation_id":"2e70536f-58c2-48a9-ba2f-64795bc61428","resolution":{"observed_at":"2026-08-14T10:58:04.901127Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.06225","last_updated":"2018-05-16T10:10:32Z","snapshot_observed_at":"2026-08-14T19:14:43.754742Z","submitted_at":"2018-05-16T10:10:32Z","title":"Determination of quark masses from $\\mathbf{n_f=4}$ lattice QCD and the RI-SMOM intermediate scheme","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.06225","snapshot_observed_at":"2026-08-14T10:58:04.905352Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.905352Z"},"links":{"cited_paper":"/paper/1805.06225","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:40cab89e3c60fe122d89aaf28ba5e99aaaa874bbb41c831e7df357cee3887bdb","observation_id":"6b7e38a9-c097-4c95-8208-dd89f153cf73","resolution":{"observed_at":"2026-08-14T10:58:04.905352Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9910332","last_updated":"2000-04-11T16:30:23Z","snapshot_observed_at":"2026-07-07T04:34:43.157892Z","submitted_at":"1999-10-13T19:42:27Z","title":"Renormalization and Running of Quark Mass and Field in the Regularization Invariant and MS-bar Schemes at Three and Four Loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9910332","snapshot_observed_at":"2026-08-14T10:58:04.909393Z","title":null,"venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.909393Z"},"links":{"cited_paper":"/paper/hep-ph/9910332","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:85d8852c19440781f336a628ffd50256c9d055d40d26b32a3e80e94c9c6bb229","observation_id":"eac2e2ab-a2d2-46bd-91b6-4f8fd04abe9d","resolution":{"observed_at":"2026-08-14T10:58:04.909393Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.4768","last_updated":"2013-05-16T18:04:23Z","snapshot_observed_at":"2026-08-15T00:35:06.877685Z","submitted_at":"2012-12-19T18:04:39Z","title":"Lattice QCD ensembles with four flavors of highly improved staggered quarks","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.4768","snapshot_observed_at":"2026-08-14T10:58:04.913354Z","title":"Bazavov et al","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.913354Z"},"links":{"cited_paper":"/paper/1212.4768","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:509036df70d7e2bccd7db82348a47a35eead59b3209d4d1d0c683fd2bcc037ff","observation_id":"8b6a52f7-fd89-49a3-a2a4-c1453fd5574a","resolution":{"observed_at":"2026-08-14T10:58:04.913354Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0304113","last_updated":"2003-04-11T14:30:44Z","snapshot_observed_at":"2026-07-07T03:59:35.126978Z","submitted_at":"2003-04-11T14:30:44Z","title":"Three loop anomalous dimension of non-singlet quark currents in the RI' scheme","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0304113","snapshot_observed_at":"2026-08-14T10:58:04.916916Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.916916Z"},"links":{"cited_paper":"/paper/hep-ph/0304113","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:f576ec3a476d5803c24caed39331eb3e93bcb28d059425b98f079d1d24d263de","observation_id":"b582788e-fd71-438c-9656-fd0113d4cc13","resolution":{"observed_at":"2026-08-14T10:58:04.916916Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.1318","last_updated":"2014-11-05T16:44:48Z","snapshot_observed_at":"2026-08-14T23:12:47.156571Z","submitted_at":"2014-11-05T16:44:48Z","title":"Radial and orbital excitation energies of charmonium","version":1},"cited_work":{"arxiv_id":"1411.1318","doi":null,"metadata_source":"pith","pith_arxiv_id":"1411.1318","snapshot_observed_at":"2026-08-14T10:58:05.012703Z","title":"Radial and orbital excitation energies of charmonium","venue":"hep-lat","work_id":"e7c68d3a-44b5-4297-90ed-68169b70d672","year":2014},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.920783Z"},"links":{"cited_paper":"/paper/1411.1318","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:bbdac8a99a6939e2ef7ea497a3964ed91d936e62e27b53c9321d0d538ae059a1","observation_id":"86954b9a-fd97-446e-8ce2-96ea6a939f95","resolution":{"observed_at":"2026-08-14T10:58:05.018561Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:58:04.924557Z","title":"Tanabashi et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.924557Z"},"links":{"citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:c0d630dab255fa9865984afe24c634cdbc62747e211c1eb16057affb025568ed","observation_id":"4c2076a3-9573-42e1-aaa5-00880e0533ef","resolution":{"observed_at":"2026-08-14T10:58:04.924557Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1208.2855","last_updated":"2012-10-17T13:11:21Z","snapshot_observed_at":"2026-08-15T00:49:55.764092Z","submitted_at":"2012-08-14T13:21:38Z","title":"Precision tests of the J/{\\psi} from full lattice QCD: mass, leptonic width and radiative decay rate to {\\eta}_c","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1208.2855","snapshot_observed_at":"2026-08-14T10:58:04.927901Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.927901Z"},"links":{"cited_paper":"/paper/1208.2855","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:8b0023909717294833e94ff7c33f5747f3561ed8aa8d4a03cb728b7588f17c62","observation_id":"a675492a-580a-44a2-a041-f0725e978396","resolution":{"observed_at":"2026-08-14T10:58:04.927901Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0907.2110","last_updated":"2015-02-10T12:18:17Z","snapshot_observed_at":"2026-08-15T05:43:52.248351Z","submitted_at":"2009-07-13T10:13:01Z","title":"Charm and Bottom Quark Masses: an Update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0907.2110","snapshot_observed_at":"2026-08-14T10:58:04.931574Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.931574Z"},"links":{"cited_paper":"/paper/0907.2110","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:cc5aea1195905f73e5a5160bf8567249f9cec5a240ecff74c0f46081fb0c5067","observation_id":"d35fd953-285d-4155-8fe1-2b7808df7705","resolution":{"observed_at":"2026-08-14T10:58:04.931574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.1778","last_updated":"2014-06-02T09:02:58Z","snapshot_observed_at":"2026-08-14T23:42:05.149198Z","submitted_at":"2014-03-07T15:26:15Z","title":"Strange and charm quark contributions to the anomalous magnetic moment of the muon","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.1778","snapshot_observed_at":"2026-08-14T10:58:04.935514Z","title":"Chakraborty et al","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.935514Z"},"links":{"cited_paper":"/paper/1403.1778","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:d1e3c2ae10e121bcdb3e31b34da7b8d94dab027f65f1cdaf748200f424742f5f","observation_id":"c885de95-3171-4ed8-8d2e-c4e77778f78b","resolution":{"observed_at":"2026-08-14T10:58:04.935514Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.04980","last_updated":"2018-07-18T10:35:52Z","snapshot_observed_at":"2026-08-14T20:13:58.303201Z","submitted_at":"2017-11-14T07:20:22Z","title":"Hadronic vacuum polarization contribution to the anomalous magnetic moments of leptons from first principles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.04980","snapshot_observed_at":"2026-08-14T10:58:04.939006Z","title":"Borsanyi et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T10:58:04.939006Z"},"links":{"cited_paper":"/paper/1711.04980","citing_paper":"/paper/1908.10116"},"observation_digest":"sha256:9dac8c2ccb6d87d40cd9ce328843238d00256d754a34871f72a20a5edbdbc088","observation_id":"035ba1d1-b60a-463f-915f-e2235a5e12f9","resolution":{"observed_at":"2026-08-14T10:58:04.939006Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.10116","last_updated":"2019-08-27T10:03:21Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-08-16T19:11:29.927613Z","submitted_at":"2019-08-27T10:03:21Z","title":"Vector current renormalisation in momentum subtraction schemes using the HISQ action"},"reference_resolution":{"displayed":14,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":13,"verified_exact":1,"verified_fuzzy":0},"total_outbound_references":14},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"thesis":"As of 16 August 2026, this Paper Citation Record lists 14 of 14 outbound references and 0 inbound Pith citation observations for arXiv:1908.10116."}