{"as_of":"2026-08-05T14:47:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:d4ac64a647275a1d96cbfdea74853cea573161e7b520983c4edb6a35147a47ff","coverage":[{"denominator":23,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":23,"source":"paper_references, paper_reference_links","source_observed_at":"2026-06-28T14:04:17.969155Z","state":"measured"},{"denominator":23,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":23,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-05T06:32:48.257954+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2606.02718/citation-record","integrity":"/paper/2606.02718/integrity","json":"/paper/2606.02718/citation-record.json","paper":"/paper/2606.02718"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:48a3561f57d354a82b0f2d506340d2404581221fff534a8983bfdc4dc30a1fd3","observation_id":"2a826b6f-761d-46a4-ad88-a67aaba17c20","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:af4db5605311aad157e3b1164594d1a029d4a0820a42bbdc4b5479e9d25bfc49","observation_id":"3c8d90a8-9e84-4994-aba9-4d8226f6f293","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"In this case the denominator∆(k)has a nonzero real constant term, so the leading threshold phase is controlled by the ratio of theO(k)imaginary term to this constant term","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:b7817043ec404d36cf79f511f1dec45ed41053292b8dd47e8f686676fff5a34b","observation_id":"cc0ab89c-604c-465d-a63a-2614d785b5de","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:7f917696b71f65393d6e00abae5cf1ee88354dc143dd04d2191f5d9b35186786","observation_id":"acd7cbe7-2dc3-4a93-848b-dee1de3c8722","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"The square-well formulas in the main text are obtained by evaluating the corresponding transfer-matrix coefficients explicitly for that model","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:f6d9c623368c67d3c97bbb7c12799c164150525234a5538b4020ec5439c5ad11","observation_id":"9f6afdb8-b1f8-40cf-96be-9cbb71336a3a","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:ebb0acf743eb0e767100951f4e331df1514c9b2796e7bc19ac5f6fd60c5a3dc7","observation_id":"b2e17651-7257-4cfc-8f85-de1850b586f4","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Büttiker and R","venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:4c5d8f7624b372f4c387e02fc8069472ad2b792f76d2b83ae054e3b61ee9070d","observation_id":"5f14315e-2296-4153-98f4-d7330381ac8f","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Landauer and T","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:51e121e812b9489b0e3525232f8585d7c52d6f026dd13af5124d367c1233f434","observation_id":"95f0af4e-065d-49b1-b5db-9329c6b0f9e3","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Muga and C","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:08c1188cf2303c0ea03daeb3fbc20108d1bef222219f4884102a002c788454a8","observation_id":"2fb2e80c-bf05-4d8a-9f3d-78eeb4cc09a7","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:1601a0224da53862eff0d6020e2356e3a6284e1d3d3f3308a5aaf8bc78a25880","observation_id":"e2363c51-0c5c-4518-8ad4-115b47f3a4a8","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:00ca02485c177a306395113b2a187df30a7d0feb50de6bc3bb53ec4bd7a3d579","observation_id":"26aefb87-52c1-4a08-bc0b-33124cda4dc7","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Salecker and E","venue":null,"work_id":null,"year":1958},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:e95f96466d24fd954a5764bdce68a5f7d654a34533f3fc9f05a5fc5739fd959b","observation_id":"ecd1b529-1f92-4e6e-a94f-e75147f54134","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Peres, Measurement of time by quantum clocks, American Journal of Physics48, 552 (1980)","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:b6c38a664793cdfdf59d2f91c2b68bfe3a6b5fae6ea6e2369e55719a45b0f786","observation_id":"53a83cf1-a14b-4410-8606-a3b59f292337","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Büttiker, Larmor precession and the traversal time for tunneling, Phys","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:99fa9ed50bfa685a4260cfa1c88d7304882a64dd4924ab04f3ad812073369dec","observation_id":"750538bb-04a9-44c0-81eb-c061b4af612b","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"tunneling time problem","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:e6748312324ed221e5fc52a4c05e5d4c6a79543fbc5409a1bbcc2e63b26d5da1","observation_id":"429999ff-c929-4261-a3d7-93f6619f684f","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:07453c16a957a61c7f0e36304235cbe9e41fd5154ee83be02030de267a7e5ddd","observation_id":"b45ef5ba-eeac-4b6c-8b2d-5ec74ab0560f","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0901.0508","last_updated":"2009-01-05T16:19:40Z","snapshot_observed_at":"2026-07-06T01:47:43.342441Z","submitted_at":"2009-01-05T16:19:40Z","title":"On the Salecker-Wigner-Peres clock and double barrier tunneling","version":1},"cited_work":{"arxiv_id":"0901.0508","doi":null,"metadata_source":"pith","pith_arxiv_id":"0901.0508","snapshot_observed_at":"2026-07-01T23:36:24.076463Z","title":"On the Salecker-Wigner-Peres clock and double barrier tunneling","venue":"quant-ph","work_id":"e95fd5cb-653a-4cfa-b2b6-462a5839dc8a","year":2009},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"cited_paper":"/paper/0901.0508","citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:ef749b60d6ea0431403ac018769094bc6c4af9e4609804246b0f4a8d8def00cf","observation_id":"a1a303c3-dce5-4f65-8bd7-f9e6e0934351","resolution":{"observed_at":"2026-07-01T23:36:24.078463Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-05T06:32:48.257954+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1108.3037","last_updated":"2011-08-15T17:25:29Z","snapshot_observed_at":"2026-07-06T02:32:26.475273Z","submitted_at":"2011-08-15T17:25:29Z","title":"Salecker-Wigner-Peres clock and average tunneling times","version":1},"cited_work":{"arxiv_id":"1108.3037","doi":null,"metadata_source":"pith","pith_arxiv_id":"1108.3037","snapshot_observed_at":"2026-07-01T23:36:24.072360Z","title":"Salecker-Wigner-Peres clock and average tunneling times","venue":"quant-ph","work_id":"6f9317ea-3b36-4c61-b1ff-a101935c5062","year":2011},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"cited_paper":"/paper/1108.3037","citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:b6d4d67a2fc0b7202efcc681c17bd96cfce744881346cab276eb8094f5b9784e","observation_id":"03dc35d8-bca9-4825-85af-8735b9ec89c0","resolution":{"observed_at":"2026-07-01T23:36:24.074343Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-05T06:32:48.257954+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":"Sokolovski, The salecker-Wigner-Peres clock, Feynman paths, and a tunnelling time that should not exist, Physical Review A96, 022120 (2017)","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:1ca5afc2d47ba8978e182f9a0127779ab9985b698d75384d3c9456d4ba652994","observation_id":"b0ade399-4d3c-4cb5-8eb5-c67bdd5aa2d7","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:47a2a93679df156584758c46c1dcf170dbdd6095ddd7f2c2b2bdb13f36ac30f0","observation_id":"f3165849-dd94-45a4-b145-5bbb4701debc","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":1960},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:0d974c0190dc3c771e8ea90aa1652f401cb1c723b0a49ea21902c932c0342951","observation_id":"f11a5ed7-21ed-41db-bbad-e305973e4898","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":1955},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:495ef3b94ace48ca0a076473e4ae7f88988cd7c35f0f5034140b9d9585afacdc","observation_id":"6b937ab1-1bc4-4652-a19b-6609678046f3","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T14:04:17.969155Z","title":null,"venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-06-28T14:04:17.969155Z"},"links":{"citing_paper":"/paper/2606.02718"},"observation_digest":"sha256:ee92760e7cbdea7728015577de8faaece0cae8ff315d5a0a9143a45ebbb8769c","observation_id":"3f77fb18-7425-4381-8b70-f3c43f7bea4d","resolution":{"observed_at":"2026-06-28T14:04:17.969155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2606.02718","last_updated":"2026-06-01T18:00:05Z","latest_version":1,"primary_category":"quant-ph","snapshot_observed_at":"2026-08-02T12:00:36.978320Z","submitted_at":"2026-06-01T18:00:05Z","title":"Resonant delay in a stationary quantum clock: Lifting the threshold mask"},"reference_resolution":{"displayed":23,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":21,"verified_exact":2,"verified_fuzzy":0},"total_outbound_references":23},"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":"2026-08-05T06:32:48.257954+00:00","source":"crossref"},{"observed_at":"2026-08-05T06:32:44.755628+00:00","source":"retraction_watch"}],"thesis":"As of 5 August 2026, this Paper Citation Record lists 23 of 23 outbound references and 0 inbound Pith citation observations for arXiv:2606.02718."}