{"as_of":"2026-08-19T08:15:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:7da0cb1648c17f7cbd3a78bba7f66a063b6f43a18561934a7cc75e6ea0a6b48e","coverage":[{"denominator":111,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T17:44:07.989889Z","state":"measured"},{"denominator":105,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":105,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-19T06:32:44.657259+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T08:32:35.017645Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-16T07:27:31.878472Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.10460","snapshot_observed_at":"2026-08-04T08:32:35.017645Z","title":"Moursy and Q","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2510.20478","last_updated":"2026-06-20T12:35:33Z","snapshot_observed_at":"2026-08-15T03:56:41.933315Z","submitted_at":"2025-10-23T12:16:57Z","title":"GUT-Scale Smooth Hybrid Inflation with a Stabilized Modulus in Light of ACT and SPT Data","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T08:32:35.017645Z"},"links":{"cited_paper":"/paper/2507.10460","citing_paper":"/paper/2510.20478"},"observation_digest":"sha256:644913b57d51df1a0e72af3ea8daa7dab6edec3369e0a8d76a246e0626a1429a","observation_id":"b77b6fc1-f87b-4b32-a3ae-a5fd8472d545","resolution":{"observed_at":"2026-08-04T08:32:35.017645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"cited_work":{"arxiv_id":"2507.10460","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.10460","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Moursy and Q","venue":null,"work_id":"c9b6bb0b-a9f5-4c5b-bc61-e1b9ed499fe0","year":2026},"citing_paper":{"arxiv_id":"2602.05623","last_updated":"2026-07-01T21:22:03Z","snapshot_observed_at":"2026-08-15T21:28:40.946696Z","submitted_at":"2026-02-05T12:58:52Z","title":"Induced-Gravity Palatini-Like Higgs Inflation in Supergravity Confronts ACT DR6","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-05-16T07:23:33.709981Z"},"links":{"cited_paper":"/paper/2507.10460","citing_paper":"/paper/2602.05623"},"observation_digest":"sha256:0c8848a155fadb65a1993f8242c4060e6c4585d54c0d191f5f94b03937ddaf4b","observation_id":"1d3a5854-a8de-4041-b863-efdbe8282a73","resolution":{"observed_at":"2026-05-16T07:27:31.880567Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.10460","snapshot_observed_at":"2026-08-03T04:22:00.883888Z","title":"Moursy and Q","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.05623","last_updated":"2026-07-01T21:22:03Z","snapshot_observed_at":"2026-08-15T21:28:40.946696Z","submitted_at":"2026-02-05T12:58:52Z","title":"Induced-Gravity Palatini-Like Higgs Inflation in Supergravity Confronts ACT DR6","version":4},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-03T04:22:00.883888Z"},"links":{"cited_paper":"/paper/2507.10460","citing_paper":"/paper/2602.05623"},"observation_digest":"sha256:13a0efca6b192a65a23397d24bdb1ad580fe78d15939ece690707906cc1bc9c2","observation_id":"0acdf35f-dbbb-456b-becf-bfe8387cd77a","resolution":{"observed_at":"2026-08-03T04:22:00.883888Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.10460","snapshot_observed_at":"2026-08-02T19:17:01.883855Z","title":"Moursy and Q","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2603.02996","last_updated":"2026-06-11T14:28:30Z","snapshot_observed_at":"2026-08-17T18:52:13.949516Z","submitted_at":"2026-03-03T13:48:25Z","title":"Magnetic monopoles and high frequency gravitational waves from quasi-stable strings","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T19:17:01.883855Z"},"links":{"cited_paper":"/paper/2507.10460","citing_paper":"/paper/2603.02996"},"observation_digest":"sha256:4e86e282e2e87e3a663354c2a820db44de5e514450eca66ea9b10b59fcf6264a","observation_id":"58f6dd2d-ee4e-49d1-8682-923839bc1598","resolution":{"observed_at":"2026-08-02T19:17:01.883855Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"cited_work":{"arxiv_id":"2507.10460","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.10460","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Moursy and Q","venue":null,"work_id":"c9b6bb0b-a9f5-4c5b-bc61-e1b9ed499fe0","year":2026},"citing_paper":{"arxiv_id":"2605.08931","last_updated":"2026-05-09T13:05:58Z","snapshot_observed_at":"2026-08-18T20:42:58.644760Z","submitted_at":"2026-05-09T13:05:58Z","title":"F-Term Hybrid Inflation with T-Model K\\\"ahler Geometry and Beyond","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-05-12T01:51:05.906605Z"},"links":{"cited_paper":"/paper/2507.10460","citing_paper":"/paper/2605.08931"},"observation_digest":"sha256:8b075e1a4a262cac31c0d8021986870d1d087bf91f51d7f829d3877bf7eb7990","observation_id":"1950ba66-f934-48f8-8b7d-af5ed50071a0","resolution":{"observed_at":"2026-05-12T01:51:14.202252Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2507.10460/citation-record","integrity":"/paper/2507.10460/integrity","json":"/paper/2507.10460/citation-record.json","paper":"/paper/2507.10460"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9406319","last_updated":"1994-06-15T17:39:45Z","snapshot_observed_at":"2026-08-19T04:15:17.760691Z","submitted_at":"1994-06-15T17:39:45Z","title":"Large Scale Structure and Supersymmetric Inflation without Fine Tuning","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9406319","snapshot_observed_at":"2026-08-06T17:44:01.752568Z","title":"Dvali, Q","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:01.752568Z"},"links":{"cited_paper":"/paper/hep-ph/9406319","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:1d41f4f8bbeb2e2fd583058082c0fb70744a151de141a948bbb3eb36e1d9c121","observation_id":"91a9e5c6-f47f-45d7-a163-2c06fcff6819","resolution":{"observed_at":"2026-08-06T17:44:01.752568Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9401011","last_updated":"1994-01-10T17:05:00Z","snapshot_observed_at":"2026-07-07T01:09:16.203858Z","submitted_at":"1994-01-10T17:05:00Z","title":"False Vacuum Inflation with Einstein Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9401011","snapshot_observed_at":"2026-08-06T17:44:01.837740Z","title":"Copeland, A.R","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:01.837740Z"},"links":{"cited_paper":"/paper/astro-ph/9401011","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:bbdb995ae2341d0ed21c68c8b376702bfdefed54056eb83472e9ca439e3ed782","observation_id":"cf1d6614-0ae0-487d-a398-f8f2c792e127","resolution":{"observed_at":"2026-08-06T17:44:01.837740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9703209","last_updated":"1997-03-14T18:33:49Z","snapshot_observed_at":"2026-08-15T18:38:20.452974Z","submitted_at":"1997-03-02T18:28:45Z","title":"Hybrid Inflation in Supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9703209","snapshot_observed_at":"2026-08-06T17:44:01.983740Z","title":"Linde and A","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:01.983740Z"},"links":{"cited_paper":"/paper/hep-ph/9703209","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:391593566505d6950d4350e1040a64d37b5ddb5c6983d98c86a339d87e723824","observation_id":"cfbf3cdc-496e-4e6e-b6ca-16e77df1f0be","resolution":{"observed_at":"2026-08-06T17:44:01.983740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.14454","last_updated":"2025-06-24T17:02:01Z","snapshot_observed_at":"2026-08-15T00:17:32.713972Z","submitted_at":"2025-03-18T17:30:26Z","title":"The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.14454","snapshot_observed_at":"2026-08-06T17:44:02.067417Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.067417Z"},"links":{"cited_paper":"/paper/2503.14454","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:0161e2289d1e0efbfe05531816ac49f8324115043ca931ed1370a215c32a8a63","observation_id":"ad60de91-b49f-4419-a865-ae1489c4b7e5","resolution":{"observed_at":"2026-08-06T17:44:02.067417Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0908.3896","last_updated":"2010-01-13T23:42:28Z","snapshot_observed_at":"2026-08-15T05:40:31.516163Z","submitted_at":"2009-08-26T20:03:02Z","title":"Supersymmetric Hybrid Inflation Redux","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0908.3896","snapshot_observed_at":"2026-08-06T17:44:02.172154Z","title":"Rehman, Q","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.172154Z"},"links":{"cited_paper":"/paper/0908.3896","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:cd7b157f368077c3b789be6ad7ef3563d8550d3d29997afaff02d6cba8b373cf","observation_id":"f2e0235e-496d-4afa-b223-613a578fc3c9","resolution":{"observed_at":"2026-08-06T17:44:02.172154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0412102","last_updated":"2005-02-25T06:23:06Z","snapshot_observed_at":"2026-07-07T04:05:57.717275Z","submitted_at":"2004-12-07T19:43:26Z","title":"Reheat temperature in supersymmetric hybrid inflation models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0412102","snapshot_observed_at":"2026-08-06T17:44:02.247858Z","title":"Senoguz and Q","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.247858Z"},"links":{"cited_paper":"/paper/hep-ph/0412102","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:aedcde5986d67ff54c91d67de8a5592692d2291452db8f4f1d429fc7ab5feb27","observation_id":"0797a9b2-4a4b-4daa-bbe8-e4c5f3c07584","resolution":{"observed_at":"2026-08-06T17:44:02.247858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9710314","last_updated":"1997-10-10T18:45:53Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1997-10-10T18:45:53Z","title":"Mu Problem and Hybrid Inflation in Supersymmetric SU(2)_L x SU(2)_R x U(1)_B-L","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9710314","snapshot_observed_at":"2026-08-06T17:44:02.318337Z","title":"Dvali, G","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.318337Z"},"links":{"cited_paper":"/paper/hep-ph/9710314","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:402d89ef776a7a641ca21a55a5fcb90de26500180e1affe362872cab9f2e944b","observation_id":"92a79eac-a411-446f-8b88-6b5f838ed063","resolution":{"observed_at":"2026-08-06T17:44:02.318337Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.1832","last_updated":"2014-07-30T16:35:23Z","snapshot_observed_at":"2026-08-14T23:38:23.036236Z","submitted_at":"2014-04-07T16:17:30Z","title":"Hybrid Inflation in the Complex Plane","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.1832","snapshot_observed_at":"2026-08-06T17:44:02.418135Z","title":"Buchmüller, V","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.418135Z"},"links":{"cited_paper":"/paper/1404.1832","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:d26617dbbc88c6d5b1148758f4f83b4eb776862eb1b89141e4233699b354a586","observation_id":"57adf54f-d9e0-4b86-b8b7-f9f42c4b4bc3","resolution":{"observed_at":"2026-08-06T17:44:02.418135Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.14831","last_updated":"2025-04-21T03:18:43Z","snapshot_observed_at":"2026-08-17T03:40:06.326560Z","submitted_at":"2025-04-21T03:18:43Z","title":"Supersymmetric Hybrid Inflation in light of Atacama Cosmology Telescope Data Release 6, Planck 2018 and LB-BK18","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.14831","snapshot_observed_at":"2026-08-06T17:44:02.483155Z","title":"Rehman and Q","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.483155Z"},"links":{"cited_paper":"/paper/2504.14831","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:f8093f2996ff6552194d76a4b7aca6670da3d34690c6eb7942b2eb82e32831d8","observation_id":"c2a68e43-3318-406b-9824-1943882cdb2c","resolution":{"observed_at":"2026-08-06T17:44:02.483155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0604198","last_updated":"2006-04-27T17:06:05Z","snapshot_observed_at":"2026-07-07T04:10:47.933399Z","submitted_at":"2006-04-24T18:08:04Z","title":"Supersymmetric Hybrid Inflation with Non-Minimal Kahler potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0604198","snapshot_observed_at":"2026-08-06T17:44:02.590042Z","title":"Bastero-Gil, S.F","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.590042Z"},"links":{"cited_paper":"/paper/hep-ph/0604198","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:1d75491083b7b5ffea46e32578f03c0fcfb97ada3dda21981410b2992aedf16f","observation_id":"92d353d0-0fc6-43a0-8db7-372acfe14c57","resolution":{"observed_at":"2026-08-06T17:44:02.590042Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0612023","last_updated":"2007-02-05T18:03:57Z","snapshot_observed_at":"2026-08-15T10:54:40.555438Z","submitted_at":"2006-12-04T17:33:18Z","title":"Supersymmetric And Smooth Hybrid Inflation In The Light Of WMAP3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0612023","snapshot_observed_at":"2026-08-06T17:44:02.630801Z","title":"ur Rehman, V.N","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.630801Z"},"links":{"cited_paper":"/paper/hep-ph/0612023","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:0c3ab2e5dd8578defd507205b2b46cef61f431911ccf218d20e9785021e5e9d7","observation_id":"98d23d54-1e33-4192-8e7c-2311eeb596fd","resolution":{"observed_at":"2026-08-06T17:44:02.630801Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.14149","last_updated":"2021-01-22T19:46:19Z","snapshot_observed_at":"2026-08-15T13:18:24.307758Z","submitted_at":"2020-09-29T16:47:36Z","title":"No-scale hybrid inflation with R-symmetry breaking","version":2},"cited_work":{"arxiv_id":"2009.14149","doi":null,"metadata_source":"pith","pith_arxiv_id":"2009.14149","snapshot_observed_at":"2026-08-06T17:44:10.317927Z","title":"No-scale hybrid inflation with R-symmetry breaking","venue":"hep-ph","work_id":"1a9a20cd-2515-4cdb-866d-70ab5fc87959","year":2020},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.700118Z"},"links":{"cited_paper":"/paper/2009.14149","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:0a06b0ef0b339a00137e3d86dc3570ae03c4d0b130720b3d091a167a6cae2a86","observation_id":"a38d0bd0-d903-4911-b235-1fee38e43a58","resolution":{"observed_at":"2026-08-06T17:44:10.323023Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2107.06670","last_updated":"2021-10-23T12:14:51Z","snapshot_observed_at":"2026-08-18T15:45:50.222797Z","submitted_at":"2021-07-14T13:00:52Z","title":"No-scale gauge non-singlet inflation inducing TeV scale inverse seesaw mechanism","version":2},"cited_work":{"arxiv_id":"2107.06670","doi":null,"metadata_source":"pith","pith_arxiv_id":"2107.06670","snapshot_observed_at":"2026-08-06T17:44:10.288693Z","title":"No-scale gauge non-singlet inflation inducing TeV scale inverse seesaw mechanism","venue":"hep-ph","work_id":"67d69076-b943-4d66-aa65-82ba99cfe24c","year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.768878Z"},"links":{"cited_paper":"/paper/2107.06670","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:9b7468cb93324733fd531dadff10fc024d7d721f851005ea23f2fcbd2c550bfe","observation_id":"c096e5c4-5fd0-463e-bbbd-c1ae310c7682","resolution":{"observed_at":"2026-08-06T17:44:10.297242Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2506.23244","last_updated":"2025-07-25T03:28:29Z","snapshot_observed_at":"2026-08-16T09:39:44.382894Z","submitted_at":"2025-06-29T14:07:45Z","title":"Supersymmetric Hybrid Inflation with K\\\"{a}hler-Induced $\\mathbf{R}$-Symmetry Breaking","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.23244","snapshot_observed_at":"2026-08-06T17:44:02.842828Z","title":"Ahmad and M.U","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.842828Z"},"links":{"cited_paper":"/paper/2506.23244","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:f57707e4daafd86c79e6377d0b0d6fbe7448b49817d41d4e879b1a69d5b3ce42","observation_id":"b97622ef-f53a-4dfa-b737-7874b52484ca","resolution":{"observed_at":"2026-08-06T17:44:02.842828Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.05564","last_updated":"2025-07-08T01:11:27Z","snapshot_observed_at":"2026-08-16T23:32:52.662119Z","submitted_at":"2025-07-08T01:11:27Z","title":"Tribrid Inflation, Type II Leptogenesis, and Observable Gravitational Waves in $SU(3)_c \\times SU(2)_L \\times SU(2)_R \\times U(1)_{B-L}$","version":1},"cited_work":{"arxiv_id":"2507.05564","doi":null,"metadata_source":"pith","pith_arxiv_id":"2507.05564","snapshot_observed_at":"2026-08-06T17:44:10.234094Z","title":"Tribrid Inflation, Type II Leptogenesis, and Observable Gravitational Waves in $SU(3)_c \\times SU(2)_L \\times SU(2)_R \\times U(1)_{B-L}$","venue":"hep-ph","work_id":"39af929b-4cda-4237-8ec1-188495a95fa5","year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:02.915184Z"},"links":{"cited_paper":"/paper/2507.05564","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6bfb50e79806799a6f02f720ac8224ac9b7022021467cd2f2161bf66472e5102","observation_id":"0c65d58f-21de-44d3-b285-7ed6b3ca1931","resolution":{"observed_at":"2026-08-06T17:44:10.240376Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+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":"2026-08-06T17:44:03.002816Z","title":"Pallis,F-Term Hybrid Inflation, Metastable Cosmic Strings and Low Reheating in View of ACT, in18th International Workshop on the Dark Side of the Universe, 4, 2025 [2504.20273]","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.002816Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:31acbb38046619f379dcf92adbec1d07aebe12c10703d9a7721a7c6e09c56bab","observation_id":"b1707842-a452-4253-b82e-cb3790b8760c","resolution":{"observed_at":"2026-08-06T17:44:03.002816Z","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":"2026-08-06T17:44:03.133672Z","title":"Okada and O","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.133672Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6ade731376618cdc593ebcb93ec9deea3c8e8618c58d97ec4612c941aec0dcfa","observation_id":"01a2b4ef-ff34-4241-a839-4b43a7707000","resolution":{"observed_at":"2026-08-06T17:44:03.133672Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1006.4522","last_updated":"2011-02-28T14:57:01Z","snapshot_observed_at":"2026-08-15T05:15:33.164591Z","submitted_at":"2010-06-23T13:57:59Z","title":"Hybrid inflation along waterfall trajectories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1006.4522","snapshot_observed_at":"2026-08-06T17:44:03.207320Z","title":"Clesse,Hybrid inflation along waterfall trajectories, Phys","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.207320Z"},"links":{"cited_paper":"/paper/1006.4522","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:60b0289000fe328c5a06bc468525d3f27f304c1c309a367acb349e2905d5a5fa","observation_id":"3be28505-6803-47b0-9b30-314dc9b40844","resolution":{"observed_at":"2026-08-06T17:44:03.207320Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1102.5612","last_updated":"2011-02-28T07:41:12Z","snapshot_observed_at":"2026-08-15T04:53:32.155628Z","submitted_at":"2011-02-28T07:41:12Z","title":"On the waterfall behavior in hybrid inflation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1102.5612","snapshot_observed_at":"2026-08-06T17:44:03.332004Z","title":"Kodama, K","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.332004Z"},"links":{"cited_paper":"/paper/1102.5612","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b3b9f41c328a92a877f0e918ce00f4b83f6404f853912dddc50b17a26b76972d","observation_id":"bf38c022-d240-430f-920a-b9ce03b5b919","resolution":{"observed_at":"2026-08-06T17:44:03.332004Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1204.3540","last_updated":"2012-06-25T08:53:35Z","snapshot_observed_at":"2026-08-15T04:12:55.306604Z","submitted_at":"2012-04-16T15:50:39Z","title":"Slow Roll during the Waterfall Regime: The Small Coupling Window for SUSY Hybrid Inflation","version":3},"cited_work":{"arxiv_id":"1204.3540","doi":null,"metadata_source":"pith","pith_arxiv_id":"1204.3540","snapshot_observed_at":"2026-08-06T17:44:10.006719Z","title":"Slow Roll during the Waterfall Regime: The Small Coupling Window for SUSY Hybrid Inflation","venue":"hep-ph","work_id":"8d0ad38e-53d7-4273-b368-f9fe387c04b1","year":2012},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.397840Z"},"links":{"cited_paper":"/paper/1204.3540","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:a9342238584efeb3e2fcd780d883e334afcbc00c2815d42d2ef705cc7603e9a0","observation_id":"84da98f6-4f5c-47cd-ae8d-15ee916c6639","resolution":{"observed_at":"2026-08-06T17:44:10.012632Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1501.07565","last_updated":"2015-01-29T19:58:34Z","snapshot_observed_at":"2026-08-16T09:59:11.642919Z","submitted_at":"2015-01-29T19:58:34Z","title":"Massive Primordial Black Holes from Hybrid Inflation as Dark Matter and the seeds of Galaxies","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.07565","snapshot_observed_at":"2026-08-06T17:44:03.476889Z","title":"Clesse and J","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.476889Z"},"links":{"cited_paper":"/paper/1501.07565","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:7a4e06a603fc31fd23e11acd1e3c10b5b6690499d71dd665951ae97ca9229694","observation_id":"c753b5ce-d11a-497b-a6f2-5f54a5a18702","resolution":{"observed_at":"2026-08-06T17:44:03.476889Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.04397","last_updated":"2024-08-31T19:53:46Z","snapshot_observed_at":"2026-08-16T13:54:38.241576Z","submitted_at":"2024-05-07T15:20:33Z","title":"Primordial monopoles, black holes and gravitational waves","version":2},"cited_work":{"arxiv_id":"2405.04397","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.04397","snapshot_observed_at":"2026-08-06T17:44:09.962868Z","title":"Primordial monopoles, black holes and gravitational waves","venue":"hep-ph","work_id":"9dfd91d4-a2da-42d3-86a9-af9096abc39d","year":2024},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.572238Z"},"links":{"cited_paper":"/paper/2405.04397","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:792d30284d3070b55049ecf0744ca4d33a52c32d57f2790190a8d3d22e2fc4e8","observation_id":"ed60578a-e26f-42f8-bff3-0db6c931535c","resolution":{"observed_at":"2026-08-06T17:44:09.968602Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2308.07094","last_updated":"2024-01-28T21:06:18Z","snapshot_observed_at":"2026-08-17T08:04:53.096992Z","submitted_at":"2023-08-14T12:05:52Z","title":"Inflation, superheavy metastable strings and gravitational waves in non-supersymmetric flipped SU(5)","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.07094","snapshot_observed_at":"2026-08-06T17:44:03.645022Z","title":"Lazarides, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.645022Z"},"links":{"cited_paper":"/paper/2308.07094","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:5e4a44a2b13e1ece914962cfd383a8e798362f81ca6442b4bed017bb0adc59d4","observation_id":"0206517e-65c7-44df-ba49-fce1fc644b25","resolution":{"observed_at":"2026-08-06T17:44:03.645022Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.13584","last_updated":"2024-12-31T18:29:23Z","snapshot_observed_at":"2026-08-17T03:32:40.164211Z","submitted_at":"2024-09-20T15:37:33Z","title":"Induced gravitational waves, metastable cosmic strings and primordial black holes in GUTs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.13584","snapshot_observed_at":"2026-08-06T17:44:03.760017Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.760017Z"},"links":{"cited_paper":"/paper/2409.13584","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:326bc23fde2e2ce7a3c670ea78199413218e41bf4034ba3ac0e898d316653fc8","observation_id":"c89a778b-9820-4864-ab9d-3bbf9cd6f6a1","resolution":{"observed_at":"2026-08-06T17:44:03.760017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.05671","last_updated":"2021-11-13T19:34:41Z","snapshot_observed_at":"2026-08-18T03:00:22.094914Z","submitted_at":"2021-08-12T11:28:15Z","title":"Gravitational Waves and Primordial Black Holes from Supersymmetric Hybrid Inflation","version":2},"cited_work":{"arxiv_id":"2108.05671","doi":null,"metadata_source":"pith","pith_arxiv_id":"2108.05671","snapshot_observed_at":"2026-08-06T17:44:09.882425Z","title":"Gravitational Waves and Primordial Black Holes from Supersymmetric Hybrid Inflation","venue":"astro-ph.CO","work_id":"5fc09d6c-2ae1-4189-814e-b7c9727a05d9","year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.831255Z"},"links":{"cited_paper":"/paper/2108.05671","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:7a08b739ffdf4f0d177c2be5439f692950a9b36d8fd9430c8f29d0ed16f8a084","observation_id":"60fbc6c6-c621-4539-a3ff-4e170593cb63","resolution":{"observed_at":"2026-08-06T17:44:09.894542Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2402.06613","last_updated":"2024-09-02T05:22:45Z","snapshot_observed_at":"2026-08-18T08:54:03.241033Z","submitted_at":"2024-02-09T18:44:36Z","title":"Primordial Black Holes and Scalar-induced Gravitational Waves in Radiative Hybrid Inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.06613","snapshot_observed_at":"2026-08-06T17:44:03.900120Z","title":"Afzal and A","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:03.900120Z"},"links":{"cited_paper":"/paper/2402.06613","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:5b31e50ec8ce42d8690840f908216cfc6b55a62a941e30f0e3e21091e9687f8a","observation_id":"21ac0a3b-82db-410e-99fe-07a01f60f1bd","resolution":{"observed_at":"2026-08-06T17:44:03.900120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.15082","last_updated":"2025-01-09T06:38:01Z","snapshot_observed_at":"2026-08-17T09:02:49.368293Z","submitted_at":"2024-07-21T07:46:33Z","title":"Primordial Black Holes and Scalar-induced Gravitational Waves in Sneutrino Hybrid Inflation","version":4},"cited_work":{"arxiv_id":"2407.15082","doi":null,"metadata_source":"pith","pith_arxiv_id":"2407.15082","snapshot_observed_at":"2026-08-06T17:44:09.830857Z","title":"Primordial Black Holes and Scalar-induced Gravitational Waves in Sneutrino Hybrid Inflation","venue":"astro-ph.CO","work_id":"0ba18322-20dc-47f5-8210-5630bea95d80","year":2024},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.005442Z"},"links":{"cited_paper":"/paper/2407.15082","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b455c4cdbabddacaa8e4bb829a48b9270cdc70349c766bb8a816a6dc7c1e9c14","observation_id":"c8c2d486-f633-4253-b8ca-2fa0cbc89cd6","resolution":{"observed_at":"2026-08-06T17:44:09.837116Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2304.01249","last_updated":"2023-06-23T07:32:18Z","snapshot_observed_at":"2026-08-18T02:02:22.127255Z","submitted_at":"2023-04-03T18:00:00Z","title":"On the primordial black hole formation in hybrid inflation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.01249","snapshot_observed_at":"2026-08-06T17:44:04.101652Z","title":"Tada and M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.101652Z"},"links":{"cited_paper":"/paper/2304.01249","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3aa612af481a157945ed96a434f49c35a32744b773b98b6f1998459a1b7f316f","observation_id":"eaefe5a4-bf79-4c1f-a494-7f4aed271d9a","resolution":{"observed_at":"2026-08-06T17:44:04.101652Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.07324","last_updated":"2023-06-12T18:00:02Z","snapshot_observed_at":"2026-08-18T04:06:33.455650Z","submitted_at":"2023-06-12T18:00:02Z","title":"Stochastic dynamics of multi-waterfall hybrid inflation and formation of primordial black holes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.07324","snapshot_observed_at":"2026-08-06T17:44:04.188593Z","title":"Tada and M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.188593Z"},"links":{"cited_paper":"/paper/2306.07324","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:71c21ad7e5ae6acf3188b7677aad9c9a780ba2605aad7459604e21692f1ddcdb","observation_id":"fde05376-a857-42dc-b119-3cf25345e5ad","resolution":{"observed_at":"2026-08-06T17:44:04.188593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.08859","last_updated":"2024-05-14T18:00:00Z","snapshot_observed_at":"2026-08-17T04:38:35.813030Z","submitted_at":"2024-05-14T18:00:00Z","title":"Multifield Stochastic Dynamics in GUT Hybrid Inflation and Gravitational Wave Signatures of GUT Higgs Representation","version":1},"cited_work":{"arxiv_id":"2405.08859","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.08859","snapshot_observed_at":"2026-08-06T17:44:09.767709Z","title":"Multifield Stochastic Dynamics in GUT Hybrid Inflation and Gravitational Wave Signatures of GUT Higgs Representation","venue":"hep-ph","work_id":"9c05ad09-b04e-45a9-9a20-8c7d21e5d97b","year":2024},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.258491Z"},"links":{"cited_paper":"/paper/2405.08859","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:887bee74b07ba2474e2f130c49d775cc22765a0315ffc3b247acae1f008092e9","observation_id":"98e9b071-e021-4f63-ac60-f2f2c576b3ea","resolution":{"observed_at":"2026-08-06T17:44:09.772893Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2211.14262","last_updated":"2023-05-10T14:37:55Z","snapshot_observed_at":"2026-08-16T16:13:17.214266Z","submitted_at":"2022-11-25T17:45:44Z","title":"Hybrid $\\alpha$-attractors, primordial black holes and gravitational wave backgrounds","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.14262","snapshot_observed_at":"2026-08-06T17:44:04.326921Z","title":"Braglia, A","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.326921Z"},"links":{"cited_paper":"/paper/2211.14262","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:811808ab005a7b0f1b4659dc089d5938e585136f9cb6eff8fae55cfbae0543f9","observation_id":"efdf5a78-049c-4ecc-8621-bb164681c84e","resolution":{"observed_at":"2026-08-06T17:44:04.326921Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9605094","last_updated":"1996-05-21T05:06:50Z","snapshot_observed_at":"2026-07-07T01:13:30.579366Z","submitted_at":"1996-05-15T23:14:21Z","title":"Density Perturbations and Black Hole Formation in Hybrid Inflation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9605094","snapshot_observed_at":"2026-08-06T17:44:04.416115Z","title":"Garcia-Bellido, A.D","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.416115Z"},"links":{"cited_paper":"/paper/astro-ph/9605094","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:e78a9862c1129b4744133f8f4ea5fbd6467cb73dba222558f9bd7a88d1e79c3f","observation_id":"2942575e-3218-45f3-b9a3-7f1b97a77da6","resolution":{"observed_at":"2026-08-06T17:44:04.416115Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0612013","last_updated":"2006-12-01T17:54:02Z","snapshot_observed_at":"2026-08-15T10:54:52.136337Z","submitted_at":"2006-12-01T17:54:02Z","title":"The cosmological gravitational wave background from primordial density perturbations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0612013","snapshot_observed_at":"2026-08-06T17:44:04.522843Z","title":"Ananda, C","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.522843Z"},"links":{"cited_paper":"/paper/gr-qc/0612013","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:2c0b57a824968d5700490c2c56cb2ef0d93545f7e6d013d03cc60ac22dde2c09","observation_id":"d9749f63-9b5b-4122-afb9-e5a21172ec36","resolution":{"observed_at":"2026-08-06T17:44:04.522843Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0703290","last_updated":"2007-03-30T19:41:36Z","snapshot_observed_at":"2026-08-15T10:43:29.653974Z","submitted_at":"2007-03-30T19:41:36Z","title":"Gravitational Wave Spectrum Induced by Primordial Scalar Perturbations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0703290","snapshot_observed_at":"2026-08-06T17:44:04.589192Z","title":"Baumann, P.J","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.589192Z"},"links":{"cited_paper":"/paper/hep-th/0703290","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:0c3f53bf02d59322d70b3e455498b25afecc7062e4108586881d814d9852b498","observation_id":"fb71fd2a-3184-431e-8e2a-f4b6f1550c6e","resolution":{"observed_at":"2026-08-06T17:44:04.589192Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.08268","last_updated":"2020-11-24T17:10:24Z","snapshot_observed_at":"2026-08-14T01:21:34.863916Z","submitted_at":"2020-09-17T13:17:48Z","title":"NANOGrav Hints to Primordial Black Holes as Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.08268","snapshot_observed_at":"2026-08-06T17:44:04.660765Z","title":"De Luca, G","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.660765Z"},"links":{"cited_paper":"/paper/2009.08268","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:689cc01f2ee5c9428cbb300496c9be6ccca1090d1d528f50427ca4460c2dff41","observation_id":"021a742c-5eea-4fb6-8352-6141305a780d","resolution":{"observed_at":"2026-08-06T17:44:04.660765Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.04189","last_updated":"2024-11-06T19:00:04Z","snapshot_observed_at":"2026-08-16T13:02:19.934154Z","submitted_at":"2024-11-06T19:00:04Z","title":"Gravitational Wave Production During Reheating: From the Inflaton to Primordial Black Holes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.04189","snapshot_observed_at":"2026-08-06T17:44:04.760218Z","title":"Gross, Y","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.760218Z"},"links":{"cited_paper":"/paper/2411.04189","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:0559df4c735eac50c2d266e54f8cca29e8739438a39a84221e0e29d4a1c1112e","observation_id":"b39f45eb-37c3-43d5-950c-61737be93b92","resolution":{"observed_at":"2026-08-06T17:44:04.760218Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.10135","last_updated":"2025-04-29T06:46:24Z","snapshot_observed_at":"2026-08-16T05:01:59.216591Z","submitted_at":"2025-02-14T13:04:41Z","title":"C-parity, magnetic monopoles and higher frequency gravitational waves","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.10135","snapshot_observed_at":"2026-08-06T17:44:04.827253Z","title":"Maji and Q","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.827253Z"},"links":{"cited_paper":"/paper/2502.10135","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:226fa6cae9ceaae7598df6f9bfdd25f5d80d635d670c26053660eb058729c2d9","observation_id":"e48271c1-fd8e-465b-ad51-af70d2352a46","resolution":{"observed_at":"2026-08-06T17:44:04.827253Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.09055","last_updated":"2025-06-25T08:04:43Z","snapshot_observed_at":"2026-08-19T03:27:53.490375Z","submitted_at":"2025-04-12T02:54:31Z","title":"Superheavy Metastable Strings in SO(10)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.09055","snapshot_observed_at":"2026-08-06T17:44:04.868098Z","title":"Maji and Q","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.868098Z"},"links":{"cited_paper":"/paper/2504.09055","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:864658ab2c70eb1245cb316536a60b744e371fd662e72a7eed40f65f2b97e0f8","observation_id":"9bd88267-637e-4009-ba34-8936ec1af29b","resolution":{"observed_at":"2026-08-06T17:44:04.868098Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.16213","last_updated":"2023-06-28T13:51:01Z","snapshot_observed_at":"2026-08-13T16:50:10.214371Z","submitted_at":"2023-06-28T13:51:01Z","title":"The NANOGrav 15-year Data Set: Evidence for a Gravitational-Wave Background","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.16213","snapshot_observed_at":"2026-08-06T17:44:04.931335Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.931335Z"},"links":{"cited_paper":"/paper/2306.16213","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b544edcba46dbe4fba7b63f1617377a05fdfea3ceb8805f7af7e7c051e19d3b0","observation_id":"66cdf2e7-9bb8-473f-a900-57e5d8700fd3","resolution":{"observed_at":"2026-08-06T17:44:04.931335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.16214","last_updated":"2023-06-28T13:51:02Z","snapshot_observed_at":"2026-08-17T09:03:17.044903Z","submitted_at":"2023-06-28T13:51:02Z","title":"The second data release from the European Pulsar Timing Array III. Search for gravitational wave signals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.16214","snapshot_observed_at":"2026-08-06T17:44:04.997765Z","title":"Search for gravitational wave signals, Astron","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:04.997765Z"},"links":{"cited_paper":"/paper/2306.16214","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:c4cb1567fcf2f758cf63f75fa9c5bd87a2fc2285319830cd6c7bc7062cf0a5a2","observation_id":"84a8e0b1-ffae-4cf0-a280-57e9f62953da","resolution":{"observed_at":"2026-08-06T17:44:04.997765Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.16216","last_updated":"2023-06-28T13:51:04Z","snapshot_observed_at":"2026-08-08T13:18:07.452026Z","submitted_at":"2023-06-28T13:51:04Z","title":"Searching for the nano-Hertz stochastic gravitational wave background with the Chinese Pulsar Timing Array Data Release I","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.16216","snapshot_observed_at":"2026-08-06T17:44:05.074268Z","title":"Xu et al.,Searching for the Nano-Hertz Stochastic Gravitational Wave Background with the Chinese Pulsar Timing Array Data Release I, Res","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.074268Z"},"links":{"cited_paper":"/paper/2306.16216","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:ea2e903e476d4051bbdce0a79def2cfc7c35462fdd932d51c9559e3752e7d891","observation_id":"68f06d11-aa56-402b-8ed3-9835e7fa3c3a","resolution":{"observed_at":"2026-08-06T17:44:05.074268Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.11320","last_updated":"2025-05-21T08:43:23Z","snapshot_observed_at":"2026-08-18T04:13:18.823853Z","submitted_at":"2025-01-20T07:47:31Z","title":"Reconstructing Primordial Curvature Perturbations via Scalar-Induced Gravitational Waves with LISA","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.11320","snapshot_observed_at":"2026-08-06T17:44:05.156200Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.156200Z"},"links":{"cited_paper":"/paper/2501.11320","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:78899ed1d38a7728cba176e6f47973be9a529b362018228022ec5de31ef05d6d","observation_id":"78328454-1753-451d-97bd-d11a1aa209b7","resolution":{"observed_at":"2026-08-06T17:44:05.156200Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.06481","last_updated":"2016-12-25T11:36:27Z","snapshot_observed_at":"2026-08-15T06:49:09.770307Z","submitted_at":"2016-10-20T16:15:02Z","title":"Science with the space-based interferometer LISA. IV: Probing inflation with gravitational waves","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.06481","snapshot_observed_at":"2026-08-06T17:44:05.196293Z","title":"Bartolo et al.,Science with the space-based interferometer LISA","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.196293Z"},"links":{"cited_paper":"/paper/1610.06481","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:8f9c74ea2a0f7fd57ba65f7d76b87f266c035417c2d29c03c4cbb9515c48665e","observation_id":"47e8efca-9ce5-4325-af5b-4117e97f0af1","resolution":{"observed_at":"2026-08-06T17:44:05.196293Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.00486","last_updated":"2021-03-19T10:41:10Z","snapshot_observed_at":"2026-08-16T19:16:32.536064Z","submitted_at":"2020-10-01T15:24:23Z","title":"ET sensitivity to the anisotropic Stochastic Gravitational Wave Background","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.00486","snapshot_observed_at":"2026-08-06T17:44:05.257082Z","title":"Mentasti and M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.257082Z"},"links":{"cited_paper":"/paper/2010.00486","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6292a1371ad7b066c0e5578c448c4dcd8a44388d1b23a3d367c853f0768eb2a9","observation_id":"195817df-edb7-4adb-bb08-cd24509326de","resolution":{"observed_at":"2026-08-06T17:44:05.257082Z","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":"2026-08-06T17:44:05.315936Z","title":"Sato et al.,The status of DECIGO, Journal of Physics: Conference Series840 (2017) 012010","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.315936Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:4fe1a2e71a9db6b02f46f427f3d6fc24581217b8021d7fc95d867e8174d55c01","observation_id":"3a031f17-4fda-4ab1-9115-ca9fcce34b92","resolution":{"observed_at":"2026-08-06T17:44:05.315936Z","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":"2026-08-06T17:44:05.366516Z","title":"Coleman and E.J","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.366516Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:29e6586e33c982801a4101e3621d4a67e02bf5f103f884c6c3f3d99e0313bbc7","observation_id":"00f9ba37-ba24-45d8-bb53-d9cf5453e848","resolution":{"observed_at":"2026-08-06T17:44:05.366516Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.04926","last_updated":"2015-11-11T10:19:29Z","snapshot_observed_at":"2026-08-18T19:44:26.841745Z","submitted_at":"2015-05-19T09:33:53Z","title":"Gravitational Waves from Double Hybrid Inflation","version":2},"cited_work":{"arxiv_id":"1505.04926","doi":null,"metadata_source":"pith","pith_arxiv_id":"1505.04926","snapshot_observed_at":"2026-08-06T17:44:09.437988Z","title":"Gravitational Waves from Double Hybrid Inflation","venue":"hep-ph","work_id":"13469a4b-044a-470f-bd28-01e7f49c545b","year":2015},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.437386Z"},"links":{"cited_paper":"/paper/1505.04926","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:44f42cd0f62dc954d2b8db44af62b4fe20c32de6c5dcb310f1d821a34ca451aa","observation_id":"5046b668-e767-4982-bb28-2af7b28bce85","resolution":{"observed_at":"2026-08-06T17:44:09.447068Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.06211","last_updated":"2019-08-02T11:42:17Z","snapshot_observed_at":"2026-08-15T10:30:26.571890Z","submitted_at":"2018-07-17T04:05:09Z","title":"Planck 2018 results. X. Constraints on inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.06211","snapshot_observed_at":"2026-08-06T17:44:05.487270Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.487270Z"},"links":{"cited_paper":"/paper/1807.06211","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3c322d4e1db2283ba30f616c26de6604996313d20472991f60bcdf87060b241f","observation_id":"10c30af9-ab40-44e7-b4f7-840e35a21eb5","resolution":{"observed_at":"2026-08-06T17:44:05.487270Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.03693","last_updated":"2017-10-04T08:00:24Z","snapshot_observed_at":"2026-08-18T18:51:46.507190Z","submitted_at":"2017-05-10T10:46:54Z","title":"$\\mu$-Hybrid Inflation with Low Reheat Temperature and Observable Gravity Waves","version":2},"cited_work":{"arxiv_id":"1705.03693","doi":null,"metadata_source":"pith","pith_arxiv_id":"1705.03693","snapshot_observed_at":"2026-08-06T17:44:09.388619Z","title":"$\\mu$-Hybrid Inflation with Low Reheat Temperature and Observable Gravity Waves","venue":"hep-ph","work_id":"5adfd908-f907-4a02-b3ad-575a203cc43c","year":2017},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.551832Z"},"links":{"cited_paper":"/paper/1705.03693","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:224ac74c8877302762ad0b483adc70ca188501d34db5476d5b3298ab832fced3","observation_id":"0ee0816c-2d2d-415b-acc2-56d4aaaeb93c","resolution":{"observed_at":"2026-08-06T17:44:09.394638Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+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":"2026-08-06T17:44:05.604261Z","title":"Kolb and M.S","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.604261Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:175125916539e003f6c5ddd327de2aa4540384b0ed062bf8ef909a482ee0b61d","observation_id":"83437f08-abdf-4b79-9a79-3df64faf03a5","resolution":{"observed_at":"2026-08-06T17:44:05.604261Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0305263","last_updated":"2003-09-11T09:08:36Z","snapshot_observed_at":"2026-08-15T09:15:34.620836Z","submitted_at":"2003-05-15T15:14:46Z","title":"How long before the end of inflation were observable perturbations produced?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0305263","snapshot_observed_at":"2026-08-06T17:44:05.660781Z","title":"Liddle and S.M","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.660781Z"},"links":{"cited_paper":"/paper/astro-ph/0305263","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b9ee501c0af3d5e34f9a10318cd8f58072e34d5459934e5cb226fc17e7f4feb3","observation_id":"88534490-35d7-45eb-a36f-90a1163a9fe1","resolution":{"observed_at":"2026-08-06T17:44:05.660781Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.06307","last_updated":"2025-04-20T14:46:40Z","snapshot_observed_at":"2026-08-16T12:59:15.828096Z","submitted_at":"2025-01-10T19:09:05Z","title":"$\\mathbf{\\mu}$-Hybrid Inflation and Metastable Cosmic Strings in $\\mathbf{SU(3)_c\\times SU(2)_L\\times SU(2)_R \\times U(1)_{B-L}}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.06307","snapshot_observed_at":"2026-08-06T17:44:05.734986Z","title":"Ahmad, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.734986Z"},"links":{"cited_paper":"/paper/2501.06307","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:51cbab6309e7dfb925d8fbd0adde42ad13c2f9f49612fe3e6d3883255f8434d6","observation_id":"1a04cfad-0bc4-489f-ba0e-0de1ca8a9b15","resolution":{"observed_at":"2026-08-06T17:44:05.734986Z","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":"2026-08-06T17:44:05.795876Z","title":"Starobinsky,Multicomponent de Sitter (Inflationary) Stages and the Generation of Perturbations, JETP Lett","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.795876Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:69cdf0228ef503b9affe91eb87eeeb69b75cf4ecebd504669be0abedc01ca544","observation_id":"6d3ce656-01cb-4ad4-bbaa-a9206e8b260e","resolution":{"observed_at":"2026-08-06T17:44:05.795876Z","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":"2026-08-06T17:44:05.844081Z","title":"Salopek and J.R","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.844081Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:16af0950f013ec39572f9222c15b98c13a484b3ace1583da56caab76a70d1117","observation_id":"12fbf121-8f2f-41a8-82a6-497d032053d4","resolution":{"observed_at":"2026-08-06T17:44:05.844081Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9507001","last_updated":"1995-11-29T04:44:50Z","snapshot_observed_at":"2026-07-07T01:11:24.120621Z","submitted_at":"1995-07-03T15:40:34Z","title":"A General Analytic Formula for the Spectral Index of the Density Perturbations produced during Inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9507001","snapshot_observed_at":"2026-08-06T17:44:05.903819Z","title":"Sasaki and E.D","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.903819Z"},"links":{"cited_paper":"/paper/astro-ph/9507001","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:f776c3af9641995b0940ff0adeebedebcecfe2134d95ad87243687e7dc11a332","observation_id":"6872ffe0-2a7f-462d-acec-cabe31190973","resolution":{"observed_at":"2026-08-06T17:44:05.903819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9801017","last_updated":"1998-03-16T06:13:27Z","snapshot_observed_at":"2026-08-06T10:43:36.599955Z","submitted_at":"1998-01-08T11:26:18Z","title":"Super-Horizon Scale Dynamics of Multi-Scalar Inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9801017","snapshot_observed_at":"2026-08-06T17:44:05.958567Z","title":"Sasaki and T","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:05.958567Z"},"links":{"cited_paper":"/paper/gr-qc/9801017","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:ce9865f72080828ed296f62af43087becbb9db5f2ac19a298a34ff5fe0b2767c","observation_id":"b1dc44eb-c31f-4238-818a-44ade3cc2b8f","resolution":{"observed_at":"2026-08-06T17:44:05.958567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0411220","last_updated":"2005-05-30T15:52:23Z","snapshot_observed_at":"2026-07-07T00:45:54.523355Z","submitted_at":"2004-11-09T11:24:00Z","title":"A general proof of the conservation of the curvature perturbation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0411220","snapshot_observed_at":"2026-08-06T17:44:06.049344Z","title":"Lyth, K.A","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.049344Z"},"links":{"cited_paper":"/paper/astro-ph/0411220","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:ed7ae5d1c0692412419966fb041cf6c118546d70290bc22ea4b97b9679e2241b","observation_id":"2b8158de-6f55-4f5e-8f40-7b7433fe0f21","resolution":{"observed_at":"2026-08-06T17:44:06.049344Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1208.1073","last_updated":"2013-02-22T15:21:20Z","snapshot_observed_at":"2026-08-15T00:50:45.385905Z","submitted_at":"2012-08-06T02:51:53Z","title":"{\\delta}N formalism","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1208.1073","snapshot_observed_at":"2026-08-06T17:44:06.116784Z","title":"Sugiyama, E","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.116784Z"},"links":{"cited_paper":"/paper/1208.1073","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:7820393d9639bd9867a631b00892ac7756c1eaa7792afec031104fa1878b9b15","observation_id":"57a7705c-d505-40fa-b4c4-3e42d8b809de","resolution":{"observed_at":"2026-08-06T17:44:06.116784Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.03515","last_updated":"2016-08-19T05:33:24Z","snapshot_observed_at":"2026-08-14T22:19:01.784782Z","submitted_at":"2015-12-11T04:12:08Z","title":"Can massive primordial black holes be produced in mild waterfall hybrid inflation?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.03515","snapshot_observed_at":"2026-08-06T17:44:06.211185Z","title":"Kawasaki and Y","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.211185Z"},"links":{"cited_paper":"/paper/1512.03515","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:856b6a9dd41c38ea6be9345cd76acaef64fb94f094a0570a3bb6d6ee47c997c5","observation_id":"1d273d71-b3dd-41d5-adc4-3f94b9637f00","resolution":{"observed_at":"2026-08-06T17:44:06.211185Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.04732","last_updated":"2016-11-30T11:03:32Z","snapshot_observed_at":"2026-08-14T22:44:20.644746Z","submitted_at":"2015-06-15T19:56:28Z","title":"Correlation Functions in Stochastic Inflation","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.04732","snapshot_observed_at":"2026-08-06T17:44:06.369599Z","title":"Vennin and A.A","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.369599Z"},"links":{"cited_paper":"/paper/1506.04732","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:731c29b8fbf73d8d04185825e02f4ce3a83ba94c7c0fa33c4a4f1fd92a7fda9a","observation_id":"ba4c23af-cd3e-469c-8435-6926e8c1e3ac","resolution":{"observed_at":"2026-08-06T17:44:06.369599Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.04502","last_updated":"2016-08-23T15:23:10Z","snapshot_observed_at":"2026-08-14T22:01:32.050666Z","submitted_at":"2016-04-15T13:48:06Z","title":"Multiple Fields in Stochastic Inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.04502","snapshot_observed_at":"2026-08-06T17:44:06.535055Z","title":"Assadullahi, H","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.535055Z"},"links":{"cited_paper":"/paper/1604.04502","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6a9106f5d2c8c65008a0691c59bb57d56858327c627b2be4a2e84948cc050acc","observation_id":"169f98f1-8d99-4ef1-8e75-7bc233f86374","resolution":{"observed_at":"2026-08-06T17:44:06.535055Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0703486","last_updated":"2015-10-07T13:54:18Z","snapshot_observed_at":"2026-08-15T10:44:28.195108Z","submitted_at":"2007-03-19T13:40:13Z","title":"The exact numerical treatment of inflationary models","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0703486","snapshot_observed_at":"2026-08-06T17:44:06.656386Z","title":"Ringeval,The exact numerical treatment of inflationary models, Lect","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.656386Z"},"links":{"cited_paper":"/paper/astro-ph/0703486","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:851ed3e180367a32030e3d4cd4eb8ccf8b31d21f5dd3d1a56150443ef3c6eaad","observation_id":"48239dea-c799-4881-a680-9d075d1b6e92","resolution":{"observed_at":"2026-08-06T17:44:06.656386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1304.7042","last_updated":"2013-12-11T22:30:49Z","snapshot_observed_at":"2026-08-15T00:19:53.799855Z","submitted_at":"2013-04-25T23:10:54Z","title":"Non-Gaussianities and Curvature Perturbations from Hybrid Inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1304.7042","snapshot_observed_at":"2026-08-06T17:44:06.831008Z","title":"Clesse, B","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.831008Z"},"links":{"cited_paper":"/paper/1304.7042","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:688badd2204386d32d40ed2aef55329e4f474b3119cec004ad2a363260ef9cf0","observation_id":"1295b090-8bb4-4e49-986a-622f09a493b3","resolution":{"observed_at":"2026-08-06T17:44:06.831008Z","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":"2026-08-06T17:44:06.935855Z","title":"Ellis, J.E","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:06.935855Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:56cec26e2af990be63130ca56497021bc523718e93e517d0d5f75ee3d99f0942","observation_id":"07a3edbe-8552-4fc9-b095-03a9e6721294","resolution":{"observed_at":"2026-08-06T17:44:06.935855Z","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":"2026-08-06T17:44:07.016883Z","title":"Moroi, H","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.016883Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:fed394311e93ae400e23e635b940faf8883bc30a176250ef31fa0c3386d4a1ee","observation_id":"57ba1dc7-eb2e-4585-b2dc-1801a8927bf7","resolution":{"observed_at":"2026-08-06T17:44:07.016883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0402490","last_updated":"2004-06-17T05:37:01Z","snapshot_observed_at":"2026-07-07T00:40:38.849273Z","submitted_at":"2004-02-20T14:18:40Z","title":"Hadronic Decay of Late-Decaying Particles and Big-Bang Nucleosynthesis","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0402490","snapshot_observed_at":"2026-08-06T17:44:07.076349Z","title":"Kawasaki, K","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.076349Z"},"links":{"cited_paper":"/paper/astro-ph/0402490","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:1e93e7be510e089b8543ad5af4cf554f9da3d27882d9ebc1a7c7b9b5b824d0ea","observation_id":"ecafc5db-1a58-42bf-a4d7-9282fd80cd18","resolution":{"observed_at":"2026-08-06T17:44:07.076349Z","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":"2026-08-06T17:44:07.175297Z","title":"Ellis, S","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.175297Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:d968796067485440b096f39d8744d43595628a282ffeb1b566655fbca7334447","observation_id":"0f88fb6f-1278-4ddd-a3a3-90b86fb94863","resolution":{"observed_at":"2026-08-06T17:44:07.175297Z","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":"2026-08-06T17:44:07.237666Z","title":"Amaldi, W","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.237666Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6a9cae47455240c55bd9485713f2d70961a9939ca44f790d7418907b9aa893e8","observation_id":"2badb207-5c5c-4a87-b7b9-72cae600a947","resolution":{"observed_at":"2026-08-06T17:44:07.237666Z","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":"2026-08-06T17:44:07.321377Z","title":"Langacker and M.-x","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.321377Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:e60a7a081de05e5005391978f72f5d2f0e7f6a99b81271252e6b1ad9a6a11a95","observation_id":"3fff52a9-adad-4c1d-b87c-7a48e11239e0","resolution":{"observed_at":"2026-08-06T17:44:07.321377Z","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":"2026-08-06T17:44:07.439731Z","title":"Amaldi, W","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.439731Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:63d25c06de43502830bdf05ec92d83af2bc3d94dc397c855b6bd7a420afa6826","observation_id":"b3884ec2-ca6f-4040-9eec-7dede8b85822","resolution":{"observed_at":"2026-08-06T17:44:07.439731Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.11391","last_updated":"2018-04-06T16:59:50Z","snapshot_observed_at":"2026-08-14T20:08:23.413005Z","submitted_at":"2017-11-30T13:48:22Z","title":"Roadmap of left-right models based on GUTs","version":2},"cited_work":{"arxiv_id":"1711.11391","doi":null,"metadata_source":"pith","pith_arxiv_id":"1711.11391","snapshot_observed_at":"2026-08-06T17:44:08.901997Z","title":"Roadmap of left-right models based on GUTs","venue":"hep-ph","work_id":"6c4f88d1-99c5-43f8-9e4a-bb04b8708c63","year":2017},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.532642Z"},"links":{"cited_paper":"/paper/1711.11391","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:fd9010bc5b302432ce95460c99b5120e1e5e04afc25edfbcd962a45de2a9689a","observation_id":"82ba99a8-088e-4641-ab75-05308e2df099","resolution":{"observed_at":"2026-08-06T17:44:08.910046Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9605054","last_updated":"1996-05-10T17:41:05Z","snapshot_observed_at":"2026-08-06T03:08:48.294553Z","submitted_at":"1996-05-10T17:41:05Z","title":"The Cosmic Microwave Background Spectrum from the Full COBE/FIRAS Data Set","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9605054","snapshot_observed_at":"2026-08-06T17:44:07.613673Z","title":"Fixsen, E.S","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.613673Z"},"links":{"cited_paper":"/paper/astro-ph/9605054","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:a0e6cd43d42d366cb5839d450f1cce610769a888cf739f8558092098bd840810","observation_id":"465a0eaf-dc7c-4a9b-9b4b-c13ee1a6e30d","resolution":{"observed_at":"2026-08-06T17:44:07.613673Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.5407","last_updated":"2014-08-08T03:07:29Z","snapshot_observed_at":"2026-08-14T23:40:27.298620Z","submitted_at":"2014-03-21T09:51:40Z","title":"Reheating the Universe Once More: The Dissipation of Acoustic Waves as a Novel Probe of Primordial Inhomogeneities on Even Smaller Scales","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.5407","snapshot_observed_at":"2026-08-06T17:44:07.689659Z","title":"Nakama, T","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.689659Z"},"links":{"cited_paper":"/paper/1403.5407","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3aa16743087ec6536e74ff00e0c76f23ade59ef7b79be742cd2ce8690f4a3d74","observation_id":"0bf7c9a1-5855-42fd-bba1-025f2276653c","resolution":{"observed_at":"2026-08-06T17:44:07.689659Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.2044","last_updated":"2011-05-10T20:14:53Z","snapshot_observed_at":"2026-08-15T04:47:10.631061Z","submitted_at":"2011-05-10T20:14:53Z","title":"The Primordial Inflation Explorer (PIXIE): A Nulling Polarimeter for Cosmic Microwave Background Observations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.2044","snapshot_observed_at":"2026-08-06T17:44:07.772147Z","title":"Kogut et al.,The Primordial Inflation Explorer (PIXIE): A Nulling Polarimeter for Cosmic Microwave Background Observations, JCAP 07 (2011) 025 [1105.2044]","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.772147Z"},"links":{"cited_paper":"/paper/1105.2044","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:773939194a3dc7a55c57a90f9afdcf5c4f09fddab5559c9997db4237da76c1ab","observation_id":"a0f53d63-32f0-4adb-8a17-8fdc1a6659ff","resolution":{"observed_at":"2026-08-06T17:44:07.772147Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.10722","last_updated":"2020-12-10T10:53:13Z","snapshot_observed_at":"2026-08-15T11:42:28.866821Z","submitted_at":"2020-07-21T11:25:21Z","title":"Primordial Black Holes as a dark matter candidate","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.10722","snapshot_observed_at":"2026-08-06T17:44:07.857190Z","title":"Green and B.J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.857190Z"},"links":{"cited_paper":"/paper/2007.10722","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:fe042a264c2a2c6876e8379f0668c51e2bd2ebb58dc188727b456e5bd3b715a7","observation_id":"82808d10-c1de-4d76-8045-a2cf5b15357e","resolution":{"observed_at":"2026-08-06T17:44:07.857190Z","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":"2026-08-06T17:44:07.862447Z","title":"’t Hooft,Magnetic Monopoles in Unified Gauge Theories, Nucl","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.862447Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:bc5d5b657324b95ea9577e54560c76034da43b7990de45b5460c89c14492bf30","observation_id":"b36c7b35-7ffe-4d38-975f-0e7f0e920fe8","resolution":{"observed_at":"2026-08-06T17:44:07.862447Z","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":"2026-08-06T17:44:07.868821Z","title":"Polyakov,Particle Spectrum in the Quantum Field Theory, JETP Lett","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.868821Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:657ecc8906208042911ee6c09c08cafb43eb0ac7e5cdcbde916e0315bdd27d32","observation_id":"8f7dbfa3-0c4a-4a35-8acd-ff86b1568dd1","resolution":{"observed_at":"2026-08-06T17:44:07.868821Z","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":"2026-08-06T17:44:07.874091Z","title":"Lazarides, M","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.874091Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b3caafa52e28334984ff36ee330d14db4affdfbe658418db9d8021b2de8d70f7","observation_id":"93cfe3e9-7054-4ac6-a8cc-0de3282a06a4","resolution":{"observed_at":"2026-08-06T17:44:07.874091Z","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":"2026-08-06T17:44:07.879764Z","title":"Shafi and C","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.879764Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3c02c45b48cfd0c80fed477fd3b74fc74082ef1d7109357c7d74dd8d9e30c078","observation_id":"d839e91b-a2e9-4b72-883d-6510c5b22f69","resolution":{"observed_at":"2026-08-06T17:44:07.879764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.08137","last_updated":"2023-03-04T06:18:00Z","snapshot_observed_at":"2026-08-17T23:29:47.336223Z","submitted_at":"2022-08-17T08:13:22Z","title":"Monopoles, Strings and Gravitational Waves in Non-minimal Inflation","version":2},"cited_work":{"arxiv_id":"2208.08137","doi":null,"metadata_source":"pith","pith_arxiv_id":"2208.08137","snapshot_observed_at":"2026-08-06T17:44:08.795992Z","title":"Monopoles, Strings and Gravitational Waves in Non-minimal Inflation","venue":"hep-ph","work_id":"7e2bd906-ad89-42e5-8f5a-838ad08af4e3","year":2022},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.884791Z"},"links":{"cited_paper":"/paper/2208.08137","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:5d7322329b40ef22e1b76cf0c7e4bdf54beb45c380bcd1ba0c8ed08c61ef1ecc","observation_id":"7252582b-428d-4e01-888f-39cd8869b088","resolution":{"observed_at":"2026-08-06T17:44:08.801904Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9802415","last_updated":"1999-05-03T13:13:27Z","snapshot_observed_at":"2026-08-05T12:37:37.908165Z","submitted_at":"1998-02-25T11:20:09Z","title":"Inflation","version":2},"cited_work":{"arxiv_id":"hep-ph/9802415","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9802415","snapshot_observed_at":"2026-08-06T17:44:08.772674Z","title":"Inflation","venue":"hep-ph","work_id":"fe7b74e9-76c2-47f6-a7ca-d3147b6486ad","year":1998},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.890174Z"},"links":{"cited_paper":"/paper/hep-ph/9802415","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:41f6472b0b9ba30dceeaac07811e56d78f2778e6110b96d569b34cf6ecb84d47","observation_id":"cd427e95-d7ac-4965-a35a-64ce7281d4c1","resolution":{"observed_at":"2026-08-06T17:44:08.778197Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0111328","last_updated":"2002-04-26T08:12:29Z","snapshot_observed_at":"2026-08-12T18:53:31.789760Z","submitted_at":"2001-11-26T10:35:50Z","title":"Inflationary Cosmology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0111328","snapshot_observed_at":"2026-08-06T17:44:07.894604Z","title":"Lazarides,Inflationary cosmology, Lect","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.894604Z"},"links":{"cited_paper":"/paper/hep-ph/0111328","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:2929ef7e436dbc29413eeda0699c2ed55eda42409c380a6dd7f97a4e9d427315","observation_id":"fb669519-4495-4ac9-a201-0eaad138cbea","resolution":{"observed_at":"2026-08-06T17:44:07.894604Z","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":"2026-08-06T17:44:07.899017Z","title":"Parker,The Origin of Magnetic Fields, Astrophys","venue":null,"work_id":null,"year":1970},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.899017Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:94602587e56f1dac8af037dd8670f2621145869ca8a6959cfb13750dad26c24d","observation_id":"3d6c0ed4-70ec-4a3c-969f-3c871cb19d87","resolution":{"observed_at":"2026-08-06T17:44:07.899017Z","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":"2026-08-06T17:44:07.903455Z","title":"Turner, E.N","venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.903455Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:07ad94b0ffe9f4e5f9614965f1222052b38c0ec4d1e2b12a1df549c571981327","observation_id":"65518eae-6485-43d3-b023-dc05edc38f66","resolution":{"observed_at":"2026-08-06T17:44:07.903455Z","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":"2026-08-06T17:44:07.907826Z","title":"Adams, M","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.907826Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b1bd7bf741578b2d5e4eb2916cbf851846aae839bb7de99cb67a1d47949212bb","observation_id":"c15abf53-bfaa-4731-bc88-123b0d654ae1","resolution":{"observed_at":"2026-08-06T17:44:07.907826Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9911095","last_updated":"1999-11-05T16:48:46Z","snapshot_observed_at":"2026-07-07T01:29:33.471797Z","submitted_at":"1999-11-05T16:48:46Z","title":"Protogalactic Extension of the Parker Bound","version":1},"cited_work":{"arxiv_id":"astro-ph/9911095","doi":null,"metadata_source":"pith","pith_arxiv_id":"astro-ph/9911095","snapshot_observed_at":"2026-08-06T17:44:08.717939Z","title":"Protogalactic Extension of the Parker Bound","venue":"astro-ph","work_id":"f4a9296a-e824-410f-b283-9ea1a81a8fd9","year":1999},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.912049Z"},"links":{"cited_paper":"/paper/astro-ph/9911095","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:27d8ca0bffde6e97089da46fb6cb2cdc4533b1ec1319142d603ec90ef1d4dee2","observation_id":"927e94b0-6bfa-42ee-ae67-b637a07effc5","resolution":{"observed_at":"2026-08-06T17:44:08.724651Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0207020","last_updated":"2002-07-09T14:49:11Z","snapshot_observed_at":"2026-07-07T03:34:45.507395Z","submitted_at":"2002-07-05T15:58:55Z","title":"Final results of magnetic monopole searches with the MACRO experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0207020","snapshot_observed_at":"2026-08-06T17:44:07.917348Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.917348Z"},"links":{"cited_paper":"/paper/hep-ex/0207020","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:41c274c49db1a0d79bbead544e807cf63ee84a2d421f277c179603ee6e482170","observation_id":"74435e35-a276-4390-8816-1ffbd1197fb2","resolution":{"observed_at":"2026-08-06T17:44:07.917348Z","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":"2026-08-06T17:44:07.922417Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.922417Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:6ad399cbd05efbdd4814241ed4cf510e29b8a00b1044c9c409ef2c40e73167cc","observation_id":"64214d03-c5fa-453e-85b7-8213b4e29226","resolution":{"observed_at":"2026-08-06T17:44:07.922417Z","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":"2026-08-06T17:44:07.930261Z","title":"Price, S.-l","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.930261Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3486bb78aa5b90e717673b13d756d5db959bbfba282b2ee9d6a75d87f78a2e26","observation_id":"b08d4db7-4d19-477a-b38d-cc6480f4019f","resolution":{"observed_at":"2026-08-06T17:44:07.930261Z","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":"2026-08-06T17:44:07.935099Z","title":"Kajita et al.,SEARCH FOR NUCLEON DECAYS CATALYZED BY MAGNETIC MONOPOLES, J","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.935099Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:9685ffb5e95a77890d9544092422d51a8142657584d696ac2cc21245623f574a","observation_id":"bb0d8d9f-f09e-43bb-8946-45ddd07a858b","resolution":{"observed_at":"2026-08-06T17:44:07.935099Z","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":"2026-08-06T17:44:07.942110Z","title":null,"venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.942110Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:8828fff5e8f4fb51f3466a36486080e5fb8f0d148227fa5ec4ac7be89be15126","observation_id":"c7a57e2f-cbe6-4c9e-9d2a-4ed3844ab0de","resolution":{"observed_at":"2026-08-06T17:44:07.942110Z","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":"2026-08-06T17:44:07.946795Z","title":"Becker-Szendy et al.,New magnetic monopole flux limits from the IMB proton decay detector, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.946795Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:cd72d50816b35b77246e6b313712f34d078cbd88540e5a18e930ce111b6ee3e1","observation_id":"aea216f3-222f-4580-8cc5-4b5b08c568e2","resolution":{"observed_at":"2026-08-06T17:44:07.946795Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0207024","last_updated":"2002-07-05T15:35:31Z","snapshot_observed_at":"2026-08-03T17:14:04.316792Z","submitted_at":"2002-07-05T15:35:31Z","title":"Search for Nucleon Decays induced by GUT Magnetic Monopoles with the MACRO Experiment","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0207024","snapshot_observed_at":"2026-08-06T17:44:07.952873Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.952873Z"},"links":{"cited_paper":"/paper/hep-ex/0207024","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3ea25e17d1a81ed068c62d680b23fc7e2b934149cc175d40b8e881f423da746d","observation_id":"bd08ea66-4bff-4ab2-a361-83a70836280c","resolution":{"observed_at":"2026-08-06T17:44:07.952873Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.0940","last_updated":"2012-03-05T15:02:11Z","snapshot_observed_at":"2026-08-15T04:17:17.364190Z","submitted_at":"2012-03-05T15:02:11Z","title":"Search for GUT Monopoles at Super-Kamiokande","version":1},"cited_work":{"arxiv_id":"1203.0940","doi":null,"metadata_source":"pith","pith_arxiv_id":"1203.0940","snapshot_observed_at":"2026-08-06T17:44:08.547665Z","title":"Search for GUT Monopoles at Super-Kamiokande","venue":"hep-ex","work_id":"ec8dd37a-df2a-4b5c-95e7-7d0e92adb520","year":2012},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.959363Z"},"links":{"cited_paper":"/paper/1203.0940","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:f8d8c5a001ef18a8584f2c9b944023004fe0b2113a5381434bf18e2b1313d278","observation_id":"2a867e2f-c1c1-47bf-8248-f6d62dadbaf8","resolution":{"observed_at":"2026-08-06T17:44:08.556588Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2202.13786","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T17:44:08.510154Z","title":null,"venue":null,"work_id":"b3d37e5b-a886-4341-a17c-44f64c367291","year":2022},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.964973Z"},"links":{"citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:c4c16c00b103a78cfc619b3b13c99996510435c83ec3886f70bf61304b2fb0a2","observation_id":"30ecc302-ce07-4dac-b6cb-a04c8036bc88","resolution":{"observed_at":"2026-08-06T17:44:08.520607Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2106.09706","last_updated":"2021-10-13T10:31:37Z","snapshot_observed_at":"2026-08-16T18:16:18.376484Z","submitted_at":"2021-06-17T17:57:53Z","title":"Escape from supercooling with or without bubbles: gravitational wave signatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.09706","snapshot_observed_at":"2026-08-06T17:44:07.969508Z","title":"Lewicki, O","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.969508Z"},"links":{"cited_paper":"/paper/2106.09706","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:007e1728e8ae82d28082bdc371531192261d1a032d10f59fc82f5144ab75ea7b","observation_id":"1c4f422e-a634-4670-a8a1-ba13269b02ba","resolution":{"observed_at":"2026-08-06T17:44:07.969508Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.08577","last_updated":"2018-06-29T02:30:22Z","snapshot_observed_at":"2026-08-14T23:23:47.705346Z","submitted_at":"2018-04-23T17:16:37Z","title":"Semianalytic Calculation of Gravitational Wave Spectrum Nonlinearly Induced from Primordial Curvature Perturbations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.08577","snapshot_observed_at":"2026-08-06T17:44:07.974846Z","title":"Kohri and T","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.974846Z"},"links":{"cited_paper":"/paper/1804.08577","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:b792ef691dfc338ef327ddf3adb51e57c1c7908de8c7d22d2ad7ede160ab15cb","observation_id":"9b97853b-8893-4666-b2a0-f6c130c9345d","resolution":{"observed_at":"2026-08-06T17:44:07.974846Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07732","last_updated":"2019-05-23T16:09:36Z","snapshot_observed_at":"2026-08-14T19:23:45.504743Z","submitted_at":"2018-04-20T17:13:45Z","title":"A Cosmological Signature of the SM Higgs Instability: Gravitational Waves","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07732","snapshot_observed_at":"2026-08-06T17:44:07.980473Z","title":"Espinosa, D","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.980473Z"},"links":{"cited_paper":"/paper/1804.07732","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:85fd0a0384814ade596365b43384d9be4e3fc55243f545e5c1db5dd93e6b0e55","observation_id":"9b6fb777-280a-4bc3-87d9-4d61a03cd629","resolution":{"observed_at":"2026-08-06T17:44:07.980473Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.00785","last_updated":"2020-01-06T09:12:01Z","snapshot_observed_at":"2026-08-19T05:26:32.371023Z","submitted_at":"2019-12-02T13:53:09Z","title":"Gauge Independence of Induced Gravitational Waves","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.00785","snapshot_observed_at":"2026-08-06T17:44:07.985300Z","title":"Inomata and T","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.985300Z"},"links":{"cited_paper":"/paper/1912.00785","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:65a2ea9eaadb56ec48e4ba44249ca284d28a7e1832949ad692eb92790d4510ee","observation_id":"9dc25932-d7e9-4e76-a0e6-55993033be55","resolution":{"observed_at":"2026-08-06T17:44:07.985300Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.00786","last_updated":"2017-02-23T05:33:01Z","snapshot_observed_at":"2026-08-17T04:50:23.618217Z","submitted_at":"2017-02-02T07:06:53Z","title":"Laser Interferometer Space Antenna","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.00786","snapshot_observed_at":"2026-08-06T17:44:07.989889Z","title":"Amaro-Seoane et al.,Laser interferometer space antenna, 1702.00786","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-06T17:44:07.989889Z"},"links":{"cited_paper":"/paper/1702.00786","citing_paper":"/paper/2507.10460"},"observation_digest":"sha256:3dc514e56c6183112d429585de2c8d7a5a693885d6c7cdd884c16004bcd59d27","observation_id":"015fefb9-dbcf-46d0-87ba-49617116d31d","resolution":{"observed_at":"2026-08-06T17:44:07.989889Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2507.10460","last_updated":"2025-07-14T16:39:06Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-15T21:45:33.219218Z","submitted_at":"2025-07-14T16:39:06Z","title":"Waterfall phase in supersymmetric hybrid inflation"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":2,"parse_uncertain":0,"unresolved":84,"verified_exact":14,"verified_fuzzy":0},"total_outbound_references":111},"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":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"thesis":"As of 19 August 2026, this Paper Citation Record lists 100 of 111 outbound references and 5 inbound Pith citation observations for arXiv:2507.10460."}