{"as_of":"2026-08-11T14:22:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:16bb235457563f07cd8e87f3277e9209edba156d06d71c68464eaf2e90874cee","coverage":[{"denominator":54,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":54,"source":"paper_references, paper_reference_links","source_observed_at":"2026-05-18T21:49:42.599333Z","state":"measured"},{"denominator":55,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":55,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-05-18T21:49:42.599333Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-05-18T21:51:52.110429Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"cited_work":{"arxiv_id":"2508.18677","doi":null,"metadata_source":"pith","pith_arxiv_id":"2508.18677","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","venue":"physics.optics","work_id":"d0e51bca-056c-437c-b35b-1288eceadcec","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"cited_paper":"/paper/2508.18677","citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:c696427becfb7e332b84ae73a685960a6da7d820661ed952665b3feeb98761f6","observation_id":"8dacd6f4-4a7c-4994-b03c-460dda457544","resolution":{"observed_at":"2026-05-18T21:51:52.113506Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2508.18677/citation-record","integrity":"/paper/2508.18677/integrity","json":"/paper/2508.18677/citation-record.json","paper":"/paper/2508.18677"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"cited_work":{"arxiv_id":"2508.18677","doi":null,"metadata_source":"pith","pith_arxiv_id":"2508.18677","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","venue":"physics.optics","work_id":"d0e51bca-056c-437c-b35b-1288eceadcec","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"cited_paper":"/paper/2508.18677","citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:c696427becfb7e332b84ae73a685960a6da7d820661ed952665b3feeb98761f6","observation_id":"8dacd6f4-4a7c-4994-b03c-460dda457544","resolution":{"observed_at":"2026-05-18T21:51:52.113506Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"elliptical polarization","venue":null,"work_id":"c192d46b-2f8f-462e-a852-dba6f7a88daa","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:feaecfe69fd6a8c20ff4a29119719be9106cd3f7938b99fad567b42ff9029303","observation_id":"b06a10ee-faad-489c-9e34-7c9c0fee434d","resolution":{"observed_at":"2026-05-18T21:51:53.227662Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"8(b) and (c) illustrating the lasing regions as functions of static electric field bias and cavity length, respectively","venue":null,"work_id":"54b92250-81ff-4397-a30a-6e02decbd7ec","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:9c501b18773a5ec9d3178489a6346a65b13078da155fb3b4460bb5bfcd95c854","observation_id":"a4b30815-c027-47f1-bf4f-9c1633e1dd62","resolution":{"observed_at":"2026-05-18T21:51:53.162568Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry phase effects on electronic properties","venue":null,"work_id":"0192fa13-e147-4d9a-9bc1-2020e17816d4","year":1959},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:021809c505dedb49e51a4065098c1c0a8bf7b7372c414c106f1d7e227461664c","observation_id":"6facd048-6caa-407a-bf9a-365ae81d9199","resolution":{"observed_at":"2026-05-18T21:51:53.166849Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Anomalous Hall effect","venue":null,"work_id":"974fa4b5-582e-4384-86ac-7ad805234c9f","year":2010},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:758ed40a78f3e39735d654fe9bceb688fe56b332d8ba9e36b5df4967d5d4cd5a","observation_id":"1a8ef336-0545-4ed7-9119-536424eb3d49","resolution":{"observed_at":"2026-05-18T21:51:53.229984Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Quantized Hall conductance in a two- dimensional periodic potential","venue":null,"work_id":"97b2b768-3515-4a85-810d-9daa7575fdf8","year":1982},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:15991bbaa6460361a2529c1c2519afaa7a336cc379eaee742f4a21dac49c0866","observation_id":"9ac45a96-ac9f-44b1-9e16-64bc9f625a8b","resolution":{"observed_at":"2026-05-18T21:51:53.294507Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Quantal phase factors accompanying adia- batic changes","venue":null,"work_id":"62a85969-5172-43b7-a21d-b6970d06e2c7","year":1984},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:6fad0c14d82503564c9f5700011ef1cb1bf45a2ee4c6e14111e8e5dfae8a4397","observation_id":"84ff9a34-8178-4c96-9549-38f2302983ef","resolution":{"observed_at":"2026-05-18T21:51:53.297751Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Colloquium: Topological band theory","venue":null,"work_id":"83175603-3d43-4bd0-bc03-b730634f086b","year":2016},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:f24ea818db2d71bbcee75fada31b1b6c306272926720c3011891c75a875bc038","observation_id":"bece8be9-bcd4-4f80-b9af-5eedea3eb0c8","resolution":{"observed_at":"2026-05-18T21:51:53.301163Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"The topology of electronic band structures","venue":null,"work_id":"7f3e4483-7f07-402f-8b9f-ae88ddb062b9","year":2021},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:5036c475986771665af7b455e17941ec97dce6fb8b37715620e967e66161b62d","observation_id":"b8011cf8-02c2-4e8e-9989-c147b179f7e9","resolution":{"observed_at":"2026-05-18T21:51:53.308270Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Quantum nonlinear Hall effect induced by Berry curvature dipole in time-reversal invari- ant materials","venue":null,"work_id":"908329ea-b1d0-4469-a564-f1e2d0a0c4fa","year":2015},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:e50b99d8b95443f9a27c65fffab8ff6cde272462361166e553521fb3d3ba2dcb","observation_id":"63abc61e-3451-495a-9fa8-2d2828cf6aec","resolution":{"observed_at":"2026-05-18T21:51:53.288549Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Band signatures for strong nonlinear Hall effect in bilayer WTe2","venue":null,"work_id":"9b7b602f-2f54-47a8-b31c-a73ac3b5ab0a","year":2018},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:edfe96dd96bc877fb976e2d4f2557cd4153426ab71aee7e5834f4f2a5bcc6352","observation_id":"7168664c-88c4-4516-84dd-c8fa699ea1f5","resolution":{"observed_at":"2026-05-18T21:51:53.270671Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Observation of the nonlinear Hall effect under time-reversal-symmetric conditions","venue":null,"work_id":"b2761c68-d3cd-4104-a243-07b04eff1b87","year":2019},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:cc69079324fc51a5f7a24b714bec947726801633099d42a54e001d067cd2633e","observation_id":"e51f44f4-463f-4d53-bbab-73b654e73983","resolution":{"observed_at":"2026-05-18T21:51:53.273486Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Field-induced Berry connection and anomalous planar Hall effect in tilted Weyl semimetals","venue":null,"work_id":"00085a36-ebd5-4fe2-870a-473d6925f2ce","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:530f269076051b593e1b4400a2ed249f893b906aac6bbb6a69fe98a52569e9cb","observation_id":"0add34e5-c5e9-425b-8900-267c43901cea","resolution":{"observed_at":"2026-05-18T21:51:53.276870Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Anomalous planar Hall effect in two-dimensional trigonal crystals","venue":null,"work_id":"2c0cb4b2-3625-42e6-8564-3d26258f9ecf","year":2021},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:eb146ab63eecfda5394d12adc5065a37b409e6553f0decafffc21f46c3b6fc6a","observation_id":"4930ead0-f5cb-48dc-af2e-9da0dc40bdde","resolution":{"observed_at":"2026-05-18T21:51:53.267240Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Quantized circular photogalvanic effect in Weyl semimetals","venue":null,"work_id":"d1da8fa2-8d1d-4a54-9beb-fccab13095d6","year":2017},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:fb333aa1acef55d04ef0950ec1f59d6d3b7351d2404f1107fa2b80e07d23c695","observation_id":"c7a28913-eb14-45d0-8d6a-966776d810b7","resolution":{"observed_at":"2026-05-18T21:51:53.279584Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Helicity-dependent photocurrents in the chiral Weyl semimetal RhSi","venue":null,"work_id":"e2d6c582-f952-41b5-85ab-ec519a740fce","year":2020},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:594f9baa73e8202a1f1ebb4f882476aca284250c569a772be0c587584a0ed02c","observation_id":"bcc37bc3-1b9c-4b70-a865-6afbf1bf4275","resolution":{"observed_at":"2026-05-18T21:51:53.291412Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Design principles for shift current photo- voltaics","venue":null,"work_id":"589c7e55-ad10-4a51-bb90-5340960dc853","year":2017},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:345cdc59066cca0646d5ed878538e211931dbeafa8badaf65e35009c21e63675","observation_id":"abf4555d-2524-4485-92f7-0c837b7f809f","resolution":{"observed_at":"2026-05-18T21:51:53.259247Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Enhanced intrinsic photovoltaic effect in tungsten disulfide nanotubes","venue":null,"work_id":"3309b083-6542-4abb-825a-76b4c699f074","year":2019},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:ca19ba0bce536dfc2ac835b35bec5770aee7b20d0385031993f83fb3dc2429d6","observation_id":"6bc72d56-49d9-4e66-a672-0983bd04c985","resolution":{"observed_at":"2026-05-18T21:51:53.264322Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Colossal mid-infrared bulk photovoltaic effect in a type-I Weyl semimetal","venue":null,"work_id":"91e065c6-c1b1-4237-8873-7a255291bbe8","year":2019},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:43ac1b8ee12c8feda24be81df4d5fc32e7f06bc61632c85483ef6080d8a53ede","observation_id":"9bead0ed-4aff-4491-854a-c86845d7ba7e","resolution":{"observed_at":"2026-05-18T21:51:53.256303Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"A van der Waals interface that creates in- plane polarization and a spontaneous photovoltaic ef- fect","venue":null,"work_id":"22e6ccbb-7546-4894-a6e5-391c0ad37875","year":2021},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:209c33cb56135d966e3a41035fed951d3257d77140a26c7fb96378a37af14d1f","observation_id":"4e187b79-1815-4b9b-9310-1b2658c3a04f","resolution":{"observed_at":"2026-05-18T21:51:53.261686Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Consequences of time-reversal-symmetry breaking in the light-matter in- teraction: Berry curvature, quantum metric, and dia- batic motion","venue":null,"work_id":"16cb900e-ea73-427d-804a-07de7ac7904b","year":2020},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:720b4798531fa8017c96e05484c943e5350faf30ad4073ee4dc91d6dfd1b5b54","observation_id":"64c6655c-27a1-454f-9663-94113741a349","resolution":{"observed_at":"2026-05-18T21:51:53.244619Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Room- temperature nonlinear Hall effect and wireless radiofre- quency rectification in Weyl semimetal TaIrTe4","venue":null,"work_id":"a1ddec71-e4b6-40be-bf41-6d3dccee8d41","year":2021},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:f3a42575db06594501d5d319f339596b53c8368434644acee266f419cae7938f","observation_id":"801f70bd-3776-4333-9d11-f211e42ae4cb","resolution":{"observed_at":"2026-05-18T21:51:53.247671Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Terahertz nonlinear Hall rectifiers based on spin- polarized topological electronic states in 1T-CoTe2","venue":null,"work_id":"be838ea8-2482-45eb-8be9-399432da161a","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:eecc6edcdc2e334ae1f2094673e2b3fb160f07cdd907bd516fba52133d2a4b17","observation_id":"a43f837c-47f1-4b9a-9c99-c3f45da6fd2e","resolution":{"observed_at":"2026-05-18T21:51:53.241601Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Nonlin- ear transport and radio frequency rectification in BiTeBr at room temperature","venue":null,"work_id":"33a53ee3-2887-436b-9e77-40543016fd9a","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:fec45e99df78b6397e21efc4a15db0cacbeb0ed001276d232f8139821ed38a0f","observation_id":"2922bd27-653e-47cd-93e9-e7f8a224e45f","resolution":{"observed_at":"2026-05-18T21:51:53.250757Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry curvature dipole senses topological transition in a moir´ e superlattice","venue":null,"work_id":"5c7aa66f-f2ed-420c-8fa1-a165a3c960d8","year":2022},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:47b11ea70325147117a2a5adbcee4014cd9320e9bb64688636b859d60266ef18","observation_id":"bbf2e281-240e-4d83-a9ce-804f376c5722","resolution":{"observed_at":"2026-05-18T21:51:53.253608Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor","venue":null,"work_id":"8e5db594-1bda-4611-bd45-b8a655f08df9","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:e0ecb47979a5b4a387f3b69744c10809cddcc7abdb4fc62d19c4531f0f1c092f","observation_id":"ad92ca4e-514c-4585-8810-860abe2276ba","resolution":{"observed_at":"2026-05-18T21:51:53.282367Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Engineering transistorlike optical gain in two-dimensional materials with Berry curva- ture dipoles","venue":null,"work_id":"5d567732-d9ba-4137-a912-c170d3a362bc","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:76803dd1bac5a40cd2adf04b724dfa237ef977be6f2472334b075dc58874e7d0","observation_id":"6531ee32-1645-4b4b-adf2-f655cd5a74fd","resolution":{"observed_at":"2026-05-18T21:51:53.285444Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Chiral terahertz lasing with Berry-curvature dipoles","venue":null,"work_id":"50c547b1-50bc-4038-a278-ca938978782f","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:d3929e2c1e1308c3c46d32afc60d100ab9177346f71d5d2ba53fa9160033cb5a","observation_id":"e82a6ee3-e004-4227-ac39-2dc8caa9474d","resolution":{"observed_at":"2026-05-18T21:51:53.304792Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2502.03399","last_updated":"2025-03-20T09:59:50Z","snapshot_observed_at":"2026-08-10T06:45:19.233764Z","submitted_at":"2025-02-05T17:36:05Z","title":"Symmetry Analysis of the Non-Hermitian Electro-Optic Effect in Crystals","version":2},"cited_work":{"arxiv_id":"2502.03399","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2502.03399","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Symmetry analysis of the non- hermitian electro-optic effect in crystals","venue":null,"work_id":"d496b2fa-0401-4f2e-b8b4-fc607d50a182","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"cited_paper":"/paper/2502.03399","citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:96354045faec6d26d911340939d47821c66c9f01e09c8e6c98052e78c1bbc1d8","observation_id":"ab6ca24a-bff3-4a3c-b88f-9a5d8c80f109","resolution":{"observed_at":"2026-05-18T21:51:52.118574Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Non-hermitian linear electro-optic effect in three-dimensional materi- als","venue":null,"work_id":"397b1046-947e-4cc3-bf69-284382679e54","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:564ffd4202d9c195cdbefac684ca637d285e60cb65421867a8326880312d595a","observation_id":"9d32c94d-58aa-4c62-be6e-7a212edc213d","resolution":{"observed_at":"2026-05-18T21:51:53.206142Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Anomalous circularly polarized light emission induced by the optical Berry curvature dipole","venue":null,"work_id":"fcbb0a4c-40a8-4954-a623-7753097b4a40","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:0940b1fc581e97e3e1b5412d398a3633403d8a3688dcac3cb4dda2f4154a2e3a","observation_id":"39df4005-d442-4f28-aeee-b655d2676faf","resolution":{"observed_at":"2026-05-18T21:51:53.311480Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Berry curvature dipole in Weyl semimetal materials: an ab initio study","venue":null,"work_id":"1c57ee3e-01cb-4c67-ada0-737a90f24d21","year":2018},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:a6eaaa2d603415fd68b5d5feccbc1e19171781dea3fb124955d9daafe7e4f759","observation_id":"3a3aea12-b2ef-4ad1-907a-c1ad4dc20021","resolution":{"observed_at":"2026-05-18T21:51:53.200376Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Optical activity in tellurium induced by a current","venue":null,"work_id":"218e1d4b-c152-4063-b7c4-ec1174011354","year":1979},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:7766f07e154a7a0c7ca7bf9b5e6a55c156bee85f8f99631ca544b07204c8c088","observation_id":"2c01081a-e082-422a-90d0-dba432a10860","resolution":{"observed_at":"2026-05-18T21:51:53.238386Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Gyrotropic effects in trigonal tellurium studied from first principles","venue":null,"work_id":"6a0255ba-a852-4bf3-9ba2-7e0fc1b5d609","year":2018},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:8633e578ccd4b61ad3f66d8e849866542540fe68ef26cc66df644070f5c1a953","observation_id":"b6ec5231-e267-42c7-bf27-1b76b211ebd9","resolution":{"observed_at":"2026-05-18T21:51:53.235565Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Topological chiral-gain in a Berry dipole material","venue":null,"work_id":"a6d4a9c4-808f-4960-90f1-8461bf4ec11b","year":2025},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:c558994b8c3c5168ee00904b839c8462be4505d185b062ab43b9b0e6593735f1","observation_id":"4d5e3738-5ed7-4b42-8a54-35040cf08219","resolution":{"observed_at":"2026-05-18T21:51:53.197753Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Space group of tellurium and selenium","venue":null,"work_id":"3e223873-82f2-49c2-bb29-9a2e4f90d3b5","year":1957},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:1b745c3ff7d0b46e102c2fa7751a4b92a5fc1c7fe1554578417dc81359a5c9dc","observation_id":"7e14998e-947a-4ec4-8074-30ca8382a92e","resolution":{"observed_at":"2026-05-18T21:51:53.202923Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Tunable chirality- dependent nonlinear electrical responses in 2D tel- lurium","venue":null,"work_id":"4adb7a78-e836-4f6f-b258-2eb3d0e1dca4","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:508f9b59132890a4b7ab238a062f65b19813b9eacf53f8a5764fa4d0c82d2104","observation_id":"0c582a5e-4913-476b-9586-2110a5a5b07b","resolution":{"observed_at":"2026-05-18T21:51:53.208882Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Chirality-tunable nonlinear Hall effect","venue":null,"work_id":"d215000f-ce59-495e-899b-ace222f2937d","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:507a1e842435dff94327b6c563cb299f02377c367bcc8856bf201d30e325e6a2","observation_id":"46238874-7ba9-403c-9910-b6c2be346bc1","resolution":{"observed_at":"2026-05-18T21:51:53.219152Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Giant nonlinear Hall and wireless rectification effects at room temperature in the elemental semiconductor tellurium","venue":null,"work_id":"16f534e1-bc5e-4169-910e-1192ae58b105","year":2024},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:bf1c2a17502d157654c11e71a53a0084869d821fe463b28ee80593aec8b1bb1b","observation_id":"a968b290-3c35-403b-8a6a-f706d4895ae9","resolution":{"observed_at":"2026-05-18T21:51:53.232611Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"High-frequency rectifica- tion via chiral bloch electrons","venue":null,"work_id":"39d350a4-3ed9-4354-830d-443fd955ad3d","year":2020},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:900a3d227b794baffd8c80404947e061ddeefaa3de93783dc1ba3ddcad16de08","observation_id":"d664ff80-1306-4567-af61-3fcd25dd9f04","resolution":{"observed_at":"2026-05-18T21:51:53.222391Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"1a3cb2e5-ef1d-457c-8813-f934f01d5342","year":null},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:a4d17dff3cfc8406279312ab914750ad5fa0e086f3f66b1fa3d59dee90b3bc14","observation_id":"2865cc8a-1f50-4838-8831-e7961e446294","resolution":{"observed_at":"2026-05-18T21:51:53.216546Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"a7a2cd3d-7787-410a-be6f-2b0cc14dafa4","year":1984},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:d22e00607b00503b0318a94efd6074b5d4e590810e40729b9d993bf37ecd33df","observation_id":"d350fa5c-9134-4b5d-bfed-928e440aa6ff","resolution":{"observed_at":"2026-05-18T21:51:53.187421Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"1358b869-a514-49e5-944c-06dcd5dc6230","year":1998},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:9ba87609b06956b7b5f576cd6314283ca7ef45bfc7b5189bf5304001e2500c00","observation_id":"8033a7c6-747c-4bf3-96ba-9cf57ef39988","resolution":{"observed_at":"2026-05-18T21:51:53.189716Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Amnon and P","venue":null,"work_id":"603881e7-a980-478b-a214-7af8c31b04ef","year":1984},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:c9361fbfca74d309df51ed8b3e86010d5fd6ad9b7a651417e0468a955b0d9206","observation_id":"7e1c4d4e-c07f-45fa-bbfb-1a106592adb3","resolution":{"observed_at":"2026-05-18T21:51:53.192051Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"79b73bc6-4864-4b55-8069-10866b86ae59","year":1973},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:3ff9e837d9de6938f6f4ed5d30cf81b8bcebdfa7d64df03aa8fc7543a0e92aff","observation_id":"72a15710-7721-4bf4-985f-65014058edff","resolution":{"observed_at":"2026-05-18T21:51:53.214156Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Versatile and active THz wave polarization modulators using metama- terial/graphene resonators","venue":null,"work_id":"a222cf74-fccf-404b-be97-bcc8f9c72b8b","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:45c0057a96b130a9b564aad4aab5747205e5cc90367c2458ff2ad282423de08f","observation_id":"561fdfd9-28f9-4670-888e-6231d08a4fd8","resolution":{"observed_at":"2026-05-18T21:51:53.211759Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Polar- ization modulation for wireless communications based on metasurfaces","venue":null,"work_id":"348d31ac-8899-4423-8220-a4a5e6f07c9d","year":2021},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:040825338a74dc8f42f7947c6c75f257ba3edc527d8e45e20bef9f5bdc0f6d05","observation_id":"d730816c-0c80-456c-9d11-4f7a85fa3379","resolution":{"observed_at":"2026-05-18T21:51:53.182552Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Opportunities and challenges in twisted bilayer graphene: a review","venue":null,"work_id":"82fb3e1e-886d-4ae2-b316-0fea3b3a4542","year":2020},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:1a00ad151e8cd7082a22a216e37adbb38cb75f38d723e1981f46f8ebeb2538d4","observation_id":"99043ac0-e8a3-4091-809e-16f1de6cd10b","resolution":{"observed_at":"2026-05-18T21:51:53.177133Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Metasurfaces-based ab- sorption and reflection control: perfect absorbers and reflectors","venue":null,"work_id":"7c5dad76-06df-42ae-bb38-6af82812a285","year":2017},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:d9a94860b663bd03a52cac6daaf4e45bef74eae812647986c34fae162efa48db","observation_id":"99343807-febc-46d3-b1f9-2b0774979154","resolution":{"observed_at":"2026-05-18T21:51:53.174363Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Switchable polarization-independent THz reflector/absorber","venue":null,"work_id":"71261b3a-3bb9-45b6-bff4-25eef140decb","year":2023},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:e73ab40a84d92bba265391230bc6f8d3ff6becdf1fdde6b25fe05033ee084c35","observation_id":"b02ee973-5e9d-430b-b4c5-86af8a30ae7e","resolution":{"observed_at":"2026-05-18T21:51:53.179895Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Relationship between intrinsic breakdown field and bandgap of materials","venue":null,"work_id":"20919472-370b-4ae7-b89a-11335db6157f","year":2006},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:8f8ab2dc1125503088d9fa6d44cd92b1d51d1149470b261bf417c15f7391724e","observation_id":"6d85f49c-d91e-4a97-80df-bb77ef4e7be3","resolution":{"observed_at":"2026-05-18T21:51:53.184971Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Negative differential con- ductivity of p-tellurium","venue":null,"work_id":"dda47bbf-2d93-4da6-90e1-6dcce5610583","year":1971},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:b34a8ec4ea2dd8b58ddb9fe3650471652d721f969f81ecc661e199ea33f80cf3","observation_id":"3dffebaa-3e95-48dd-ab62-2ce0c76f00d9","resolution":{"observed_at":"2026-05-18T21:51:53.194901Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Current-induced spin polarization of holes in tellurium","venue":null,"work_id":"0522e963-64ad-495d-9563-48acfd99e8d0","year":2012},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:8c834860dcd32418255a6ecdc427db6ed74f22101611c79c6403b6223813b3dd","observation_id":"7937450f-1203-42c8-bd0a-441617a703f1","resolution":{"observed_at":"2026-05-18T21:51:53.225145Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"High-field transport and low-field mobility in tellurium single crys- tals","venue":null,"work_id":"8ab4a516-33b2-4695-a5bb-6d653162c5ea","year":1973},"citing_paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-05-18T21:49:42.599333Z"},"links":{"citing_paper":"/paper/2508.18677"},"observation_digest":"sha256:365bf5a4f5bbe3bd81eff28fb5994df26b05cdf09e0737d9f7fda95bd10f4563","observation_id":"4e7a1c4a-36fb-42c3-8f7b-4f0ae2f138fe","resolution":{"observed_at":"2026-05-18T21:51:53.171331Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2508.18677","last_updated":"2026-01-27T20:13:59Z","latest_version":2,"primary_category":"physics.optics","snapshot_observed_at":"2026-07-06T22:18:40.868747Z","submitted_at":"2025-08-26T04:48:26Z","title":"Berry Curvature Dipole-Induced Chiral Terahertz Gain and Lasing Threshold in Bulk Tellurium"},"reference_resolution":{"displayed":54,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":4,"verified_exact":2,"verified_fuzzy":48},"total_outbound_references":54},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 54 of 54 outbound references and 1 inbound Pith citation observation for arXiv:2508.18677."}