{"as_of":"2026-08-23T02:25:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:dc9a0c7931efed6b92b4b1791d82559b6caed0916e9df4416094a3c191c1976b","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":"2026-08-14T14:05:32.583776Z","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":"2026-08-22T06:32:14.747728+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/1908.03824/citation-record","integrity":"/paper/1908.03824/integrity","json":"/paper/1908.03824/citation-record.json","paper":"/paper/1908.03824"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T14:05:32.794679Z","title":"In order to describe the particle guiding center motion, we follow the canonical Hamiltonian equations 28","venue":null,"work_id":"12d10695-022c-40c8-ab2e-2f5db0790019","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.527688Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:e9b7fc4cea143e33ac86644dff93fc562e393f2e7fdbae22b29a0f4249a663ef","observation_id":"e3a078f6-3bf0-4ead-af53-739f262e998a","resolution":{"observed_at":"2026-08-14T14:05:32.799294Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.781949Z","title":"(16) The dominant terms of the equations of motion are obtained by omitting the terms of the order of ρ∗ =ρth/a and ofBθ/B, whereρth =mvth/(ZeB), vth = √ 2T/m","venue":null,"work_id":"f3136583-3422-45ac-846e-37a67d3b572a","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.533007Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:3ea8d46c33504cb3163164d5a0e652c6494703ddc0015e26a25463399084eb1d","observation_id":"0e57bb0f-bfea-4ef7-b84a-9717001f3dec","resolution":{"observed_at":"2026-08-14T14:05:32.786388Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.768988Z","title":"Generally, E× B drift vE is contributed from the equilibrium scalar potential δφeq and the perturbed scalar potential δφ, i.e., vE = vE,eq +δvE","venue":null,"work_id":"93b91e80-481d-4368-846b-c0297290abe3","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.537363Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:0525c7a088e9a44aa696d9a696d14d092f3758925c2bc4e8bd6ed95275b8cc14","observation_id":"1f320d86-9f91-446e-a030-1e4c8abdf4cc","resolution":{"observed_at":"2026-08-14T14:05:32.773459Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.756586Z","title":"(22) The dominant term is ˙v‖0≈−µ(bR∂RB +bZ∂ZB)","venue":null,"work_id":"e3aa4522-4964-4a89-9c2a-123e43b8e842","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.541851Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:e4b5eb166b8d46999de80194f09f69a0b8f6a20ce51438e4121459bc5043dd7f","observation_id":"07ff6f9c-5d78-4489-b394-72a001dad793","resolution":{"observed_at":"2026-08-14T14:05:32.760425Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.744640Z","title":null,"venue":null,"work_id":"e4915371-b2de-4ee7-978c-94ad0332a88a","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.546198Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:bc88afecee923356941b0b69b743b0eff1b591857a6475d114cd739d33b618d5","observation_id":"4293ea4e-dabf-4acc-9477-67f04f99c7d4","resolution":{"observed_at":"2026-08-14T14:05:32.748418Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.731252Z","title":"The field equation is solved using the finite element method for unstructured meshes","venue":null,"work_id":"3e969a87-9c6e-447e-bc7d-206aa4769c59","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.550646Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:24c642076ccd2d457ce1620247e4364caff64adf00c7687c04747ec548f23fa7","observation_id":"bebc178d-995c-461f-9a21-8dad6b09fecc","resolution":{"observed_at":"2026-08-14T14:05:32.735601Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.717809Z","title":"charge deposition","venue":null,"work_id":"8e8024e2-9052-4232-83b6-bac0cdd0fe31","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.555389Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:0eede9ee3f6b1d5d58d97f070562e32d393ed95709d7c0cd7d5a29082f830f66","observation_id":"27df32f3-802c-4513-9a23-5b71d3e2d756","resolution":{"observed_at":"2026-08-14T14:05:32.721997Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.704028Z","title":"17, 21 and 23, are solved","venue":null,"work_id":"a7324a68-c2a1-4ce7-87b7-48b9628405c8","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.559676Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:e4c1a30d875bea492716d1d46be77a836feb16c99a4bcab071898acc830b9abb","observation_id":"8151fa53-00ad-452c-abe3-5d7adac26108","resolution":{"observed_at":"2026-08-14T14:05:32.708804Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.690011Z","title":"33, is ignored","venue":null,"work_id":"8ad76f56-1449-4cb1-a88e-a5635877c258","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.563679Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:cf0bf8aa572178077f969fc1537f0d54b88213e460f5389bc591ddb0dd36eb3e","observation_id":"78cb7bd7-de90-4692-adf8-0063b8ef6cb2","resolution":{"observed_at":"2026-08-14T14:05:32.694317Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.676375Z","title":"40 for the weight equation is kept but the equilibrium variation in n, T and B is omitted","venue":null,"work_id":"25c5d53a-8e83-4723-9e37-bd96f2f722c8","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.567834Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:4f499f7b01c4bfd9c3fa9aee31ef9572b62157a2f5320b0b36f0eedb6ed97cd3","observation_id":"7b77306b-db67-4369-877b-a60f9feaede2","resolution":{"observed_at":"2026-08-14T14:05:32.680906Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.662714Z","title":null,"venue":null,"work_id":"34d8952d-7ec8-48f2-ac93-6a13fdb7d074","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.571870Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:905fc5afabcd6745690bcde0a56e5aa6c2e7231ca9e52e5c1ddb279fa5a4c4b1","observation_id":"60bb1698-b30d-406b-bfac-7b18e0fed1c3","resolution":{"observed_at":"2026-08-14T14:05:32.666752Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.648307Z","title":"absorbing boundary condition","venue":null,"work_id":"f0ffcfe4-ab66-4ecb-b743-f8c58b5aa3a9","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.575858Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:0779104fe1f587dd3975f2e841ffbb68827d731dc074a8df0cca4b69ed4fa592","observation_id":"0b985107-659d-4a06-83a1-ae7b827b06b1","resolution":{"observed_at":"2026-08-14T14:05:32.652366Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+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":"2026-08-14T14:05:32.635043Z","title":null,"venue":null,"work_id":"accfac7f-2499-4a41-b84f-8b4b988cb840","year":null},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.579880Z"},"links":{"citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:5ad601931933560a9e4c4b593fda777ed298cb541c271d28514573d4a1ac9aae","observation_id":"0b843129-c779-4765-91ef-1c9dad1fb696","resolution":{"observed_at":"2026-08-14T14:05:32.639249Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1905.01906","last_updated":"2019-05-06T10:03:28Z","snapshot_observed_at":"2026-08-14T16:36:50.636301Z","submitted_at":"2019-05-06T10:03:28Z","title":"ORB5: a global electromagnetic gyrokinetic code using the PIC approach in toroidal geometry","version":1},"cited_work":{"arxiv_id":"1905.01906","doi":null,"metadata_source":"pith","pith_arxiv_id":"1905.01906","snapshot_observed_at":"2026-08-14T14:05:32.618765Z","title":"ORB5: a global electromagnetic gyrokinetic code using the PIC approach in toroidal geometry","venue":"physics.plasm-ph","work_id":"f8d0738c-e2f7-4551-b469-bcc96e160b78","year":2019},"citing_paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:32.583776Z"},"links":{"cited_paper":"/paper/1905.01906","citing_paper":"/paper/1908.03824"},"observation_digest":"sha256:9824542d7caa5b466bfcbb8f0d0b3abc14d0c71677a9df40cffdbb71cdf4bb06","observation_id":"a3368d1c-ae57-4a96-92f3-b59be3a9db94","resolution":{"observed_at":"2026-08-14T14:05:32.624724Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"1908.03824","last_updated":"2020-07-14T10:10:15Z","latest_version":2,"primary_category":"physics.plasm-ph","snapshot_observed_at":"2026-08-16T09:34:43.175426Z","submitted_at":"2019-08-10T22:52:24Z","title":"Development and testing of an unstructured mesh method for whole plasma gyrokinetic simulations in realistic tokamak geometry"},"reference_resolution":{"displayed":14,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":3,"verified_exact":1,"verified_fuzzy":10},"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":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 14 of 14 outbound references and 0 inbound Pith citation observations for arXiv:1908.03824."}