{"as_of":"2026-08-12T15:34:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:2d7912b3f34fbc5819c6198f868489910ca392f08b0ef339325759d04c6175cb","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":12,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":12,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-12T06:34:41.77262+00:00","state":"measured"},{"denominator":12,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":12,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T19:17:06.507988Z","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":"2026-07-04T05:19:34.805208Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-10T19:17:06.507988Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2501.10532","last_updated":"2025-02-10T22:29:56Z","snapshot_observed_at":"2026-08-11T04:03:43.650336Z","submitted_at":"2025-01-17T20:13:15Z","title":"Bayesian Inferring Nucleon's Gravitation Form Factors via Near-threshold $J/\\psi$ Photoproduction","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-10T19:17:06.507988Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2501.10532"},"observation_digest":"sha256:9401c7d533c362c8c5a8eb86e21c1e73ee92b11ced81263220a112c4891f59ae","observation_id":"04888c7a-b3c1-43aa-b969-0a3793376e48","resolution":{"observed_at":"2026-08-10T19:17:06.507988Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-07T05:36:19.785454Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.07554","last_updated":"2025-06-09T08:47:30Z","snapshot_observed_at":"2026-08-10T01:00:09.335659Z","submitted_at":"2025-06-09T08:47:30Z","title":"Proton Gravitational Structure and Mass Decomposition on the Light Front","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-07T05:36:19.785454Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2506.07554"},"observation_digest":"sha256:fd530c9bbfdd15f5c88a1470c0bb55ba479ea9a764bac076e1c2ed30a69f1c4a","observation_id":"48084966-4756-4c97-a06f-063277726df1","resolution":{"observed_at":"2026-08-07T05:36:19.785454Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-06T15:55:07.900020Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.14840","last_updated":"2025-08-22T18:58:55Z","snapshot_observed_at":"2026-08-09T16:14:24.936774Z","submitted_at":"2025-07-20T06:53:09Z","title":"Mechanical properties of the $\\Omega^-$ baryon from gravitational form factors","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T15:55:07.900020Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2507.14840"},"observation_digest":"sha256:06289eb29d160ddf346d627fc2d78d5b10deb825bfd812405496043629e4d4d0","observation_id":"235277c8-746e-42d8-8635-7d3e4c3758b3","resolution":{"observed_at":"2026-08-06T15:55:07.900020Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-06T13:07:41.624250Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.21220","last_updated":"2026-06-07T12:42:44Z","snapshot_observed_at":"2026-08-06T13:07:39.674824Z","submitted_at":"2025-07-28T18:00:02Z","title":"Gravitational form factors of the nucleon in the Skyrme model based on scale-invariant chiral perturbation theory","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T13:07:41.624250Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2507.21220"},"observation_digest":"sha256:49cd3aaf8b7fc641648c82061ae564f7a72ffa51d5f157652e01f08903dc9d7d","observation_id":"9e8e2924-7aad-45cc-8897-134c15f066c2","resolution":{"observed_at":"2026-08-06T13:07:41.624250Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-03T20:29:57.279344Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2511.20715","last_updated":"2026-05-22T19:15:15Z","snapshot_observed_at":"2026-08-12T14:13:32.543103Z","submitted_at":"2025-11-25T02:52:59Z","title":"Mechanical properties of the proton from a deformed AdS holographic model","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T20:29:57.279344Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2511.20715"},"observation_digest":"sha256:d4a93edb1dd8ba1c3d06d69811b93f6c44ab196e8aba89a177ac254af21f497c","observation_id":"99c87e1c-f144-4c4c-9eaf-0e4a83b257a3","resolution":{"observed_at":"2026-08-03T20:29:57.279344Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-03T16:08:29.430367Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.15064","last_updated":"2026-07-30T01:23:49Z","snapshot_observed_at":"2026-08-07T08:52:29.813125Z","submitted_at":"2025-12-17T04:04:16Z","title":"Three-dimensional imaging of hadrons with hard exclusive reactions: advances in experiment, theory, phenomenology, and lattice QCD","version":5},"reference_index":215,"source":"pdf_text","source_observed_at":"2026-08-03T16:08:29.430367Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2512.15064"},"observation_digest":"sha256:6e5984948a3b573a019ec361c1918fb37985b5a141d1b6298952f037360e5522","observation_id":"12684b02-2ac8-4faa-841a-af3604b9af50","resolution":{"observed_at":"2026-08-03T16:08:29.430367Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-03T15:17:03.292265Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2512.17554","last_updated":"2026-07-25T02:38:58Z","snapshot_observed_at":"2026-08-12T15:14:02.811518Z","submitted_at":"2025-12-19T13:22:29Z","title":"Proton Structure from a Soft-Wall Holographic QCD Model: Mass Spectrum, Form Factors, and Mechanical Properties","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-03T15:17:03.292265Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2512.17554"},"observation_digest":"sha256:4415d6526b14902cd14824df94f73c50bcec5a50b7a0309ab2b12b4ed4e5000d","observation_id":"8a21f3b3-43cb-407b-b1e3-c7b43bac746a","resolution":{"observed_at":"2026-08-03T15:17:03.292265Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-08-02T19:15:42.372020Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2603.03064","last_updated":"2026-06-04T16:17:26Z","snapshot_observed_at":"2026-08-07T03:53:18.157682Z","submitted_at":"2026-03-03T15:03:21Z","title":"Momentum-projected hadron entanglement from lattice-QCD replica correlators","version":4},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-02T19:15:42.372020Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2603.03064"},"observation_digest":"sha256:b972c6d3495e749fa5114b4046e88520b49c993e51e5b3527d8ad94edb3607ed","observation_id":"35db5ce6-b53d-4620-a74f-94ed6cbbba48","resolution":{"observed_at":"2026-08-02T19:15:42.372020Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":"1910.04707","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-07-04T05:19:34.805208Z","title":"Diﬀractive photoproduction of J/ψ and Υ using holo- graphic QCD: gravitational form factors and GPD of gluons in the proton","venue":null,"work_id":"029150c6-4a46-4d05-9732-21de7dadd382","year":2020},"citing_paper":{"arxiv_id":"2604.12038","last_updated":"2026-06-15T18:44:13Z","snapshot_observed_at":"2026-07-12T21:36:58.184763Z","submitted_at":"2026-04-13T20:26:23Z","title":"Holographic Open/Closed Exchange in Double Deeply Virtual Compton Scattering: Fixed-$j$ Structural Matching to the $\\pm$-Basis Wilson Kernels","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-10T15:00:17.970696Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2604.12038"},"observation_digest":"sha256:b726328d3715925ae1198350011be9be6ece54243b6c8fd7256ecb2180537b50","observation_id":"42801a81-3c31-4849-8281-90362f6c6d45","resolution":{"observed_at":"2026-05-11T11:21:02.647985Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":"1910.04707","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-07-04T05:19:34.805208Z","title":"Diﬀractive photoproduction of J/ψ and Υ using holo- graphic QCD: gravitational form factors and GPD of gluons in the proton","venue":null,"work_id":"029150c6-4a46-4d05-9732-21de7dadd382","year":2020},"citing_paper":{"arxiv_id":"2604.20247","last_updated":"2026-07-15T06:53:48Z","snapshot_observed_at":"2026-08-11T11:00:42.922571Z","submitted_at":"2026-04-22T06:50:04Z","title":"Near-Threshold OPE Constraints and High-Energy Diffractive Dynamics in J/psi Photoproduction","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-10T00:30:41.676337Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2604.20247"},"observation_digest":"sha256:48f344347303ceaaed31e6e7b8a563e93c5bf370edfa34060a720bccdbdd166e","observation_id":"6d873e2e-1e9d-4942-8418-fa9454a2b412","resolution":{"observed_at":"2026-05-11T13:46:05.732056Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":"1910.04707","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-07-04T05:19:34.805208Z","title":"Diﬀractive photoproduction of J/ψ and Υ using holo- graphic QCD: gravitational form factors and GPD of gluons in the proton","venue":null,"work_id":"029150c6-4a46-4d05-9732-21de7dadd382","year":2020},"citing_paper":{"arxiv_id":"2606.20981","last_updated":"2026-06-18T23:16:18Z","snapshot_observed_at":"2026-07-06T23:56:02.397254Z","submitted_at":"2026-06-18T23:16:18Z","title":"Gluon GTMD at strong coupling: fixed-spin saddle factorization and Reggeization","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-06-26T16:11:36.369423Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2606.20981"},"observation_digest":"sha256:9ec31379f1a2289b27c3bf62d9fe4136bec96c88f5345cc9372db89f7bccadbb","observation_id":"da677538-9002-49df-8b22-3a041b39d36c","resolution":{"observed_at":"2026-07-04T05:19:34.806998Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04707","snapshot_observed_at":"2026-07-31T01:28:52.415577Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.25099","last_updated":"2026-07-27T21:54:56Z","snapshot_observed_at":"2026-08-05T14:39:28.197326Z","submitted_at":"2026-07-27T21:54:56Z","title":"Spin resummation of heavy quarkonium photoproduction: from the gluonic gravitational form factors to the holographic pomeron","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-07-31T01:28:52.415577Z"},"links":{"cited_paper":"/paper/1910.04707","citing_paper":"/paper/2607.25099"},"observation_digest":"sha256:00b24fc3c99faaae77dbe67247f7628171bd67a1890b14a55a31db8501a4c6cd","observation_id":"69d58487-57ea-4344-b66b-e07075c30973","resolution":{"observed_at":"2026-07-31T01:28:52.415577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1910.04707/citation-record","integrity":"/paper/1910.04707/integrity","json":"/paper/1910.04707/citation-record.json","paper":"/paper/1910.04707"},"outbound":[],"paper":{"arxiv_id":"1910.04707","last_updated":"2019-10-10T17:04:16Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-09T02:45:06.981346Z","submitted_at":"2019-10-10T17:04:16Z","title":"Diffractive photoproduction of $J/\\psi$ and $\\Upsilon$ using holographic QCD: gravitational form factors and GPD of gluons in the proton"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"thesis":"As of 12 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 12 inbound Pith citation observations for arXiv:1910.04707."}