{"as_of":"2026-08-10T15:12:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:a421e4e13e530f5444c108223c8fde3fd33d3ef024aa7419bfe3fe6c2178cc9d","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":24,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":24,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":24,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":24,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T11:21:32.551580Z","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":"2026-07-04T01:29:22.861196Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"1907.04324","last_updated":"2019-07-09T15:47:40Z","snapshot_observed_at":"2026-08-02T21:52:17.274751Z","submitted_at":"2019-07-09T15:47:40Z","title":"Dark Matter Energy Deposition and Production from the Table-Top to the Cosmos","version":1},"reference_index":265,"source":"pdf_text","source_observed_at":"2026-05-25T00:19:36.048465Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/1907.04324"},"observation_digest":"sha256:7457b16e552e6858eb768622ac4ebe7d968bb046be9c3371f091a086bd6c765f","observation_id":"cdfe0cda-bcc9-4dcb-a4c4-69a6667f7b7f","resolution":{"observed_at":"2026-05-25T00:20:07.202545Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-07T11:21:32.551580Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2506.02910","last_updated":"2026-05-23T11:07:08Z","snapshot_observed_at":"2026-08-07T11:10:22.136247Z","submitted_at":"2025-06-03T14:15:29Z","title":"About electroweak domain walls in Majoron models","version":4},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-07T11:21:32.551580Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2506.02910"},"observation_digest":"sha256:0d156faad8bbbe0b2b423eb4d98a26127d542f4d3604f92175361405d0c038db","observation_id":"f393becd-abe4-4e3d-a655-a3468fa15984","resolution":{"observed_at":"2026-08-07T11:21:32.551580Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2506.23290","last_updated":"2026-04-17T09:16:11Z","snapshot_observed_at":"2026-07-06T21:49:24.430655Z","submitted_at":"2025-06-29T15:26:07Z","title":"Type II Seesaw Leptogenesis in a Majoron background","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-05-19T07:47:44.372827Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2506.23290"},"observation_digest":"sha256:403dff80c53367e50bda4559191798e34b22befaed9f64d1b4969f8e50ba5e1b","observation_id":"f6c15b56-48de-4ed1-94b3-4099f0d9ef02","resolution":{"observed_at":"2026-05-19T07:52:10.142127Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-06T18:59:27.010987Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.07180","last_updated":"2025-07-09T18:00:03Z","snapshot_observed_at":"2026-08-09T13:27:42.683826Z","submitted_at":"2025-07-09T18:00:03Z","title":"Exploring Quantum Statistics for Dirac and Majorana Neutrinos using Spinor-Helicity techniques","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T18:59:27.010987Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2507.07180"},"observation_digest":"sha256:2026c1f44f7ad570d6ff375085a7a69137f345b013cc04b3814e2ada6ad3cbe5","observation_id":"ebe7e36e-d5b2-41e5-bb35-0624511a5e47","resolution":{"observed_at":"2026-08-06T18:59:27.010987Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-06T17:18:01.051449Z","title":"Dreiner, H.E","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.11426","last_updated":"2025-07-15T15:51:23Z","snapshot_observed_at":"2026-08-09T15:20:12.732318Z","submitted_at":"2025-07-15T15:51:23Z","title":"UV completions of scalar-tensor EFTs","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T17:18:01.051449Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2507.11426"},"observation_digest":"sha256:5a3ace0a6bd1792d53931ea140956acc6e8d9b05a4006d7c795936ed89730cee","observation_id":"2e774fcf-1e94-4df6-b557-68e9467de769","resolution":{"observed_at":"2026-08-06T17:18:01.051449Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-05T17:21:44.540831Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2508.16724","last_updated":"2025-08-22T18:00:24Z","snapshot_observed_at":"2026-08-09T06:43:04.118232Z","submitted_at":"2025-08-22T18:00:24Z","title":"Searching for neutrino polarizability at DUNE","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-05T17:21:44.540831Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2508.16724"},"observation_digest":"sha256:33b4cf24a29e1a44efc5bd3adf87322cd0ef071b7a8a920d1a0d6a77d5d2db1a","observation_id":"60c2998c-1f0b-4892-9ff7-661b1c72de14","resolution":{"observed_at":"2026-08-05T17:21:44.540831Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2509.24680","last_updated":"2026-04-13T11:17:37Z","snapshot_observed_at":"2026-07-06T22:31:05.409865Z","submitted_at":"2025-09-29T12:16:13Z","title":"Lepton number violating signals of a parity symmetric model at $\\mu$TRISTAN","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-18T12:58:21.085023Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2509.24680"},"observation_digest":"sha256:1ecd6bfc6ced65b4eb2102e63ddf6e3e7a009539d4d1e17b2831c355ff3075a5","observation_id":"2c5e8e71-933c-4c57-9a1e-a1b2f0d2af0d","resolution":{"observed_at":"2026-05-18T13:01:23.825693Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-03T17:24:16.346271Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2512.10015","last_updated":"2026-06-01T15:42:32Z","snapshot_observed_at":"2026-08-08T07:17:13.995398Z","submitted_at":"2025-12-10T19:07:01Z","title":"The Four Polarizations of the $W$ at High Energies","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T17:24:16.346271Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2512.10015"},"observation_digest":"sha256:de884d3f129709762050dd1c5be6501074c496d9ddf768c5f15f680cb776090d","observation_id":"223597a4-b4e4-4f76-8c29-051c35939bd2","resolution":{"observed_at":"2026-08-03T17:24:16.346271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-03T14:47:22.750122Z","title":"Dreiner, H.E","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2512.19833","last_updated":"2026-06-04T18:03:26Z","snapshot_observed_at":"2026-08-07T19:52:33.770335Z","submitted_at":"2025-12-22T19:43:20Z","title":"Universal Seesaw Leptogenesis","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-03T14:47:22.750122Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2512.19833"},"observation_digest":"sha256:67e9f0a3b3463e794b3d2b0788d1bdf42209d60aa327486bbf07c6700c322b16","observation_id":"99310623-ae8a-489d-8fd5-cfa3dc793ba4","resolution":{"observed_at":"2026-08-03T14:47:22.750122Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2604.06929","last_updated":"2026-04-16T08:22:39Z","snapshot_observed_at":"2026-07-06T22:55:20.208897Z","submitted_at":"2026-04-08T10:41:40Z","title":"Direct-detection constraints on inelastic dark matter with a scalar mediator","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-05-10T17:36:54.459136Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2604.06929"},"observation_digest":"sha256:1ebc3fb822e72329121850141c6be7c3bb3ac1e6dcc44b573cfa02ce2324ac19","observation_id":"42d738f2-2cc6-41b4-8799-16f75f2f5b0a","resolution":{"observed_at":"2026-05-11T06:30:59.775701Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2604.20385","last_updated":"2026-04-22T09:39:06Z","snapshot_observed_at":"2026-07-06T23:06:49.210284Z","submitted_at":"2026-04-22T09:39:06Z","title":"Prospects of boosted magnetic dipole inelastic fermion dark matter at ILC-BDX","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-05-10T00:36:45.703898Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2604.20385"},"observation_digest":"sha256:5d7c03b8ac6c4fc910413658aa71cdc15c89f94c55b2c3a63bb198a24332e933","observation_id":"643c2e01-361f-48ad-bed9-e41840ef67d5","resolution":{"observed_at":"2026-05-11T13:46:04.875346Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2604.25989","last_updated":"2026-04-28T18:00:00Z","snapshot_observed_at":"2026-07-06T23:11:43.764239Z","submitted_at":"2026-04-28T18:00:00Z","title":"EFT Pathways to $|\\Delta B| =2$: Chiral Constructions and Phenomenology","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-05-07T15:42:33.980801Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2604.25989"},"observation_digest":"sha256:79b73a59f6735a3e99f9cdab5a9d71972c258206169c99cb0745afae06f7f35b","observation_id":"6244a738-75a8-4793-84c1-e88e21853280","resolution":{"observed_at":"2026-05-12T00:11:15.904049Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2605.07516","last_updated":"2026-05-08T09:46:37Z","snapshot_observed_at":"2026-07-06T23:19:51.414344Z","submitted_at":"2026-05-08T09:46:37Z","title":"Collinear matching for leading power gluon transverse momentum distributions","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-05-11T02:21:40.151753Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.07516"},"observation_digest":"sha256:add1691c2b93b40be0459bd33acb1de37cb395229f6fdf260ccdc780ab2d3af3","observation_id":"287ffeb4-155b-4f6c-8e9f-6956264b6683","resolution":{"observed_at":"2026-05-11T03:45:55.494481Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2605.15176","last_updated":"2026-05-14T17:57:40Z","snapshot_observed_at":"2026-07-30T06:05:28.057811Z","submitted_at":"2026-05-14T17:57:40Z","title":"Matching higher-dimensional operators at finite temperature for general models","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-05-15T02:57:53.925105Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.15176"},"observation_digest":"sha256:a54744b6a93afec79ef74d419560f182d65f2212330f1c99f60d5420991db990","observation_id":"0162cc12-5232-4441-b4cf-754f874db3a0","resolution":{"observed_at":"2026-05-15T02:58:34.074429Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2605.21419","last_updated":"2026-07-07T19:09:59Z","snapshot_observed_at":"2026-07-12T16:18:15.917852Z","submitted_at":"2026-05-20T17:13:10Z","title":"Cosmological Collider Signatures from Right-Handed Neutrino Loop","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-05-21T03:41:07.257985Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.21419"},"observation_digest":"sha256:ccb95f47adf42c203ca38d5a245a9adbf1e80adfaf7823105900c3b94ad24e07","observation_id":"03a55653-88d8-4492-b905-73b2c4e7af9c","resolution":{"observed_at":"2026-05-21T03:43:56.441178Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-12T16:18:19.288976Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2605.21419","last_updated":"2026-07-07T19:09:59Z","snapshot_observed_at":"2026-07-12T16:18:15.917852Z","submitted_at":"2026-05-20T17:13:10Z","title":"Cosmological Collider Signatures from Right-Handed Neutrino Loop","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-07-12T16:18:19.288976Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.21419"},"observation_digest":"sha256:d5ca2bd48c3815b4c74fc9033cbc523bd347d09c8063156e4e8ac0ac32d9c72c","observation_id":"8ea68370-5752-495c-b978-f1bd4deac78a","resolution":{"observed_at":"2026-07-12T16:18:19.288976Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2605.24126","last_updated":"2026-05-22T18:38:10Z","snapshot_observed_at":"2026-08-07T11:01:49.047024Z","submitted_at":"2026-05-22T18:38:10Z","title":"Resonant Enhancement for the transfer of baryon number from a CP-violating hidden sector","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-06-30T15:48:40.690558Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.24126"},"observation_digest":"sha256:2fc2ff02c029164ac31e44f5d99fd3e5f74d8281dcdda7166a925f96411f764f","observation_id":"16b8b91e-dfc4-4014-b908-e9020cb22bd1","resolution":{"observed_at":"2026-06-30T15:54:49.525709Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2605.28054","last_updated":"2026-05-27T06:59:43Z","snapshot_observed_at":"2026-07-06T23:37:40.695655Z","submitted_at":"2026-05-27T06:59:43Z","title":"Fermionic Bubble Loop in Cosmological Collider Revisited: Exact signals from spectral and Mellin-Barnes methods","version":1},"reference_index":123,"source":"pdf_text","source_observed_at":"2026-06-29T11:29:32.957501Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2605.28054"},"observation_digest":"sha256:d417040f4bd695b1fa85362fdba35a693dc956589da7a1dce6d5ffc2d665f66a","observation_id":"8e232c37-d1db-4bbf-89fa-6d5a3543579d","resolution":{"observed_at":"2026-06-29T12:23:24.884554Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2606.18641","last_updated":"2026-06-17T03:26:00Z","snapshot_observed_at":"2026-08-07T14:15:28.939449Z","submitted_at":"2026-06-17T03:26:00Z","title":"SUSY meets pseudo-Hermiticity","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-06-26T20:19:18.110426Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2606.18641"},"observation_digest":"sha256:673606b986fddba55b55b8bfd3103af6a507049c0df361eb24453fc964cbcfb8","observation_id":"c4641270-4061-4e79-be34-a27abae81cbd","resolution":{"observed_at":"2026-07-04T01:29:22.862468Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":"0812.1594","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-04T01:29:22.861196Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","venue":null,"work_id":"cbbcd96f-26b5-4393-ab91-51bb56e6a8df","year":2010},"citing_paper":{"arxiv_id":"2606.28496","last_updated":"2026-06-26T18:00:08Z","snapshot_observed_at":"2026-08-02T10:51:07.253060Z","submitted_at":"2026-06-26T18:00:08Z","title":"Polarization interference in exclusive $V+$jets at all orders in $\\alpha_s$","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-06-30T00:50:55.495498Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2606.28496"},"observation_digest":"sha256:ab7bb857abfadaa983577eb1febb6931a15716befb36f721417894712982d654","observation_id":"fb7946f6-55b1-48aa-9aad-e2dc72a5d1cb","resolution":{"observed_at":"2026-07-01T16:15:49.270635Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-07-11T07:06:40.243456Z","title":"Two- Component Spinor Techniques and Feynman Rules for Quantum Field Theory and Supersymmetry,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2607.05485","last_updated":"2026-07-06T17:56:57Z","snapshot_observed_at":"2026-08-09T15:07:01.972518Z","submitted_at":"2026-07-06T17:56:57Z","title":"An inquiry on the Absence of Fermion Doubling and why the Nielsen-Ninomiya Theorem Does Not Apply to Nonlocal Quantum Field Theory","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-07-11T07:06:40.243456Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2607.05485"},"observation_digest":"sha256:d453e243ac60362b68bd0b87b1c352428b63f31af992c10e37f57171e2eee602","observation_id":"c9afb9ef-2744-4c42-9917-a42fc8208d7c","resolution":{"observed_at":"2026-07-11T07:06:40.243456Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-01T15:36:44.165211Z","title":"Dreiner, H.E","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2607.18398","last_updated":"2026-07-20T18:00:12Z","snapshot_observed_at":"2026-08-09T07:43:04.223145Z","submitted_at":"2026-07-20T18:00:12Z","title":"The fermion sector of the SMEFT from asymptotically safe gravity","version":1},"reference_index":146,"source":"pdf_text","source_observed_at":"2026-08-01T15:36:44.165211Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2607.18398"},"observation_digest":"sha256:93a16c2c29060edc58e7b67e5823e39237d51987fc19ed511308791320f27063","observation_id":"0b756026-9174-4f9f-b002-92e13df51554","resolution":{"observed_at":"2026-08-01T15:36:44.165211Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-01T14:42:51.809333Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2607.18708","last_updated":"2026-07-21T05:04:22Z","snapshot_observed_at":"2026-08-08T07:50:38.166011Z","submitted_at":"2026-07-21T05:04:22Z","title":"LFV decays in a 3-3-1 model with singlet leptoquarks","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-01T14:42:51.809333Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2607.18708"},"observation_digest":"sha256:f492c36d75440b633c93c4cc572700cf3a1774e7d92ef305484b87a280d4c8ea","observation_id":"58d51df7-137a-4aae-9307-7900ddbf1867","resolution":{"observed_at":"2026-08-01T14:42:51.809333Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1594","snapshot_observed_at":"2026-08-04T01:13:49.099589Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2608.00166","last_updated":"2026-07-31T18:00:01Z","snapshot_observed_at":"2026-08-07T04:39:30.473203Z","submitted_at":"2026-07-31T18:00:01Z","title":"The flavour of SU(15) composite quarks and leptons","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T01:13:49.099589Z"},"links":{"cited_paper":"/paper/0812.1594","citing_paper":"/paper/2608.00166"},"observation_digest":"sha256:825dfb81bcefe55a1cd147a48b8099d67f2068003f934de87c95afbc128eb90d","observation_id":"e8d93c34-8cae-4b00-9329-1e5931980516","resolution":{"observed_at":"2026-08-04T01:13:49.099589Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/0812.1594/citation-record","integrity":"/paper/0812.1594/integrity","json":"/paper/0812.1594/citation-record.json","paper":"/paper/0812.1594"},"outbound":[],"paper":{"arxiv_id":"0812.1594","last_updated":"2022-05-24T09:22:41Z","latest_version":6,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-08T17:15:26.165328Z","submitted_at":"2008-12-09T20:49:40Z","title":"Two-component spinor techniques and Feynman rules for quantum field theory and supersymmetry"},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 24 inbound Pith citation observations for arXiv:0812.1594."}