{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:WUKGSVAYSMOCTEA32YICKL2Z5K","short_pith_number":"pith:WUKGSVAY","canonical_record":{"source":{"id":"2505.09202","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-14T07:28:01Z","cross_cats_sorted":["astro-ph.CO","hep-ex"],"title_canon_sha256":"9d9b845bfc155c51514bf5fc099be035dbaf29e3a87765d50aba8750afc54f97","abstract_canon_sha256":"735ee71ead241328c19db8da58d6a9911996c6ddf281b5b017e006d7f4e9f6c3"},"schema_version":"1.0"},"canonical_sha256":"b514695418931c29901bd610252f59eabb0080fcb99674483c027e2e602f3794","source":{"kind":"arxiv","id":"2505.09202","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.09202","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"arxiv_version","alias_value":"2505.09202v3","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.09202","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_12","alias_value":"WUKGSVAYSMOC","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_16","alias_value":"WUKGSVAYSMOCTEA3","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_8","alias_value":"WUKGSVAY","created_at":"2026-06-19T16:11:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:WUKGSVAYSMOCTEA32YICKL2Z5K","target":"record","payload":{"canonical_record":{"source":{"id":"2505.09202","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-14T07:28:01Z","cross_cats_sorted":["astro-ph.CO","hep-ex"],"title_canon_sha256":"9d9b845bfc155c51514bf5fc099be035dbaf29e3a87765d50aba8750afc54f97","abstract_canon_sha256":"735ee71ead241328c19db8da58d6a9911996c6ddf281b5b017e006d7f4e9f6c3"},"schema_version":"1.0"},"canonical_sha256":"b514695418931c29901bd610252f59eabb0080fcb99674483c027e2e602f3794","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-19T16:11:10.907476Z","signature_b64":"sVqpTiH1qBVWfI79l+6b6I0JnCe1g8IwyO5hiuhJEHhlyTPMqFAeLg34HLY+NYOa+ep9MpvBmyBqM6bliNnaCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b514695418931c29901bd610252f59eabb0080fcb99674483c027e2e602f3794","last_reissued_at":"2026-06-19T16:11:10.907115Z","signature_status":"signed_v1","first_computed_at":"2026-06-19T16:11:10.907115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2505.09202","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-19T16:11:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IepDKAa9vURIGDwIJoRxdVk6NJaKH5+mfzgwOKGZPXwvuJrsBcUvdZcsSS6k10mqI6DCeIqWTHEsfLclrizXDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:21:51.539803Z"},"content_sha256":"770989b4d2686dfbe4be9dfdfdcf945bfcc225afa9dd0dfaa9d63d2be1d556e2","schema_version":"1.0","event_id":"sha256:770989b4d2686dfbe4be9dfdfdcf945bfcc225afa9dd0dfaa9d63d2be1d556e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:WUKGSVAYSMOCTEA32YICKL2Z5K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Angular momentum of vacuum bubbles in a first-order phase transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions","cross_cats":["astro-ph.CO","hep-ex"],"primary_cat":"hep-ph","authors_text":"Danny Marfatia, Jan Tristram Acu\\~na, Po-Yan Tseng","submitted_at":"2025-05-14T07:28:01Z","abstract_excerpt":"The formation of primordial black holes (PBHs) during a first-order phase transition (FOPT) in a dark sector has been of recent interest. A quantity that characterizes a black hole is its spin. We carry out the first step towards determining the spin of such PBHs, by calculating the spin of spherical false vacuum bubbles induced by cosmological perturbations. The angular momentum is given by the product of density and velocity perturbations. We carefully track the evolution of background quantities and calculate the transfer functions during the FOPT. We find that the dimensionless spin parame"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"The dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles of mass M and angular momentum J take a wide range of values from O(10^{-5}) to O(10) for FOPTs between 10 keV and 100 GeV and a dark sector that is 0.1 to 0.4 times cooler than the visible sector. A scaling relation exists between the root-mean-square value of the spin, the FOPT time scale, the bubble wall velocity, and the dark sector-to-visible sector temperature ratio.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"Angular momentum of the bubbles is given exactly by the product of density and velocity perturbations, with bubbles remaining spherical while background quantities and transfer functions are tracked through the FOPT; this modeling choice is stated as the basis for the calculation in the abstract.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Computes the dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles from density and velocity perturbations in FOPTs, yielding values from O(10^{-5}) to O(10) and a scaling relation with FOPT timescale, wall velocity, and temperature ratio.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"3d38bfcf61de8d6968afecb73b2264a20846002cd9560469e572ec45f6934956"},"source":{"id":"2505.09202","kind":"arxiv","version":3},"verdict":{"id":"4cb7013b-435f-47b9-a2fb-8f35c44c1329","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-22T15:58:24.965857Z","strongest_claim":"The dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles of mass M and angular momentum J take a wide range of values from O(10^{-5}) to O(10) for FOPTs between 10 keV and 100 GeV and a dark sector that is 0.1 to 0.4 times cooler than the visible sector. A scaling relation exists between the root-mean-square value of the spin, the FOPT time scale, the bubble wall velocity, and the dark sector-to-visible sector temperature ratio.","one_line_summary":"Computes the dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles from density and velocity perturbations in FOPTs, yielding values from O(10^{-5}) to O(10) and a scaling relation with FOPT timescale, wall velocity, and temperature ratio.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"Angular momentum of the bubbles is given exactly by the product of density and velocity perturbations, with bubbles remaining spherical while background quantities and transfer functions are tracked through the FOPT; this modeling choice is stated as the basis for the calculation in the abstract.","pith_extraction_headline":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions"},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.09202/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":62,"sample":[{"doi":"","year":1974,"title":"W.H. Press and P. Schechter,Formation of galaxies and clusters of galaxies by selfsimilar gravitational condensation,Astrophys. J.187(1974) 425","work_id":"c4ba41f5-0a98-49d5-9c85-d0c32fb8f5e4","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2004,"title":"A new calculation of the mass fraction of primordial black holes","work_id":"e7a7c0f5-75b9-4311-9891-7a33b5f3fb13","ref_index":2,"cited_arxiv_id":"astro-ph/0403181","is_internal_anchor":true},{"doi":"","year":2020,"title":"S. Young and M. Musso,Application of peaks theory to the abundance of primordial black holes, JCAP11(2020) 022 [2001.06469]","work_id":"752ab54b-386a-42bc-9fc6-97cc160a9543","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2021,"title":"C.-M. Yoo, T. Harada, S. Hirano and K. Kohri,Abundance of Primordial Black Holes in Peak Theory for an Arbitrary Power Spectrum,PTEP2021(2021) 013E02 [2008.02425]","work_id":"4c46f2bf-ea75-404a-924c-5a2915cc5344","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2020,"title":"M. Mirbabayi, A. Gruzinov and J. Nore˜ na,Spin of Primordial Black Holes,JCAP03(2020) 017 [1901.05963]","work_id":"a0e63472-e279-41e1-a985-97319b7f44c8","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":62,"snapshot_sha256":"f9bae1858219d225fa205626929b1ad4aea9eea85a117bd253d3216056f5398d","internal_anchors":19},"formal_canon":{"evidence_count":2,"snapshot_sha256":"564405ccb717560f81cd5281727b74d9912b43510f9f4fa8ab91e1982a0a44b2"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"4cb7013b-435f-47b9-a2fb-8f35c44c1329"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-19T16:11:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XmusNMLssLmcvS4RzMavaosLE0AncSqc5fHQY7pUtEVnhWd+295i1/BgR5H0S9jQfqjqc4P3S/m+rJWPevL3Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:21:51.541304Z"},"content_sha256":"402ffb655e2d799c844ed2d4e42cb883c66536eb20b289b7ea60a2530f6e3a14","schema_version":"1.0","event_id":"sha256:402ffb655e2d799c844ed2d4e42cb883c66536eb20b289b7ea60a2530f6e3a14"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/bundle.json","state_url":"https://pith.science/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-05T01:21:51Z","links":{"resolver":"https://pith.science/pith/WUKGSVAYSMOCTEA32YICKL2Z5K","bundle":"https://pith.science/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/bundle.json","state":"https://pith.science/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WUKGSVAYSMOCTEA32YICKL2Z5K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:WUKGSVAYSMOCTEA32YICKL2Z5K","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"735ee71ead241328c19db8da58d6a9911996c6ddf281b5b017e006d7f4e9f6c3","cross_cats_sorted":["astro-ph.CO","hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-14T07:28:01Z","title_canon_sha256":"9d9b845bfc155c51514bf5fc099be035dbaf29e3a87765d50aba8750afc54f97"},"schema_version":"1.0","source":{"id":"2505.09202","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.09202","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"arxiv_version","alias_value":"2505.09202v3","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.09202","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_12","alias_value":"WUKGSVAYSMOC","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_16","alias_value":"WUKGSVAYSMOCTEA3","created_at":"2026-06-19T16:11:10Z"},{"alias_kind":"pith_short_8","alias_value":"WUKGSVAY","created_at":"2026-06-19T16:11:10Z"}],"graph_snapshots":[{"event_id":"sha256:402ffb655e2d799c844ed2d4e42cb883c66536eb20b289b7ea60a2530f6e3a14","target":"graph","created_at":"2026-06-19T16:11:10Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"The dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles of mass M and angular momentum J take a wide range of values from O(10^{-5}) to O(10) for FOPTs between 10 keV and 100 GeV and a dark sector that is 0.1 to 0.4 times cooler than the visible sector. A scaling relation exists between the root-mean-square value of the spin, the FOPT time scale, the bubble wall velocity, and the dark sector-to-visible sector temperature ratio."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"Angular momentum of the bubbles is given exactly by the product of density and velocity perturbations, with bubbles remaining spherical while background quantities and transfer functions are tracked through the FOPT; this modeling choice is stated as the basis for the calculation in the abstract."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Computes the dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles from density and velocity perturbations in FOPTs, yielding values from O(10^{-5}) to O(10) and a scaling relation with FOPT timescale, wall velocity, and temperature ratio."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions"}],"snapshot_sha256":"3d38bfcf61de8d6968afecb73b2264a20846002cd9560469e572ec45f6934956"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"564405ccb717560f81cd5281727b74d9912b43510f9f4fa8ab91e1982a0a44b2"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2505.09202/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The formation of primordial black holes (PBHs) during a first-order phase transition (FOPT) in a dark sector has been of recent interest. A quantity that characterizes a black hole is its spin. We carry out the first step towards determining the spin of such PBHs, by calculating the spin of spherical false vacuum bubbles induced by cosmological perturbations. The angular momentum is given by the product of density and velocity perturbations. We carefully track the evolution of background quantities and calculate the transfer functions during the FOPT. We find that the dimensionless spin parame","authors_text":"Danny Marfatia, Jan Tristram Acu\\~na, Po-Yan Tseng","cross_cats":["astro-ph.CO","hep-ex"],"headline":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-14T07:28:01Z","title":"Angular momentum of vacuum bubbles in a first-order phase transition"},"references":{"count":62,"internal_anchors":19,"resolved_work":62,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"W.H. Press and P. Schechter,Formation of galaxies and clusters of galaxies by selfsimilar gravitational condensation,Astrophys. J.187(1974) 425","work_id":"c4ba41f5-0a98-49d5-9c85-d0c32fb8f5e4","year":1974},{"cited_arxiv_id":"astro-ph/0403181","doi":"","is_internal_anchor":true,"ref_index":2,"title":"A new calculation of the mass fraction of primordial black holes","work_id":"e7a7c0f5-75b9-4311-9891-7a33b5f3fb13","year":2004},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"S. Young and M. Musso,Application of peaks theory to the abundance of primordial black holes, JCAP11(2020) 022 [2001.06469]","work_id":"752ab54b-386a-42bc-9fc6-97cc160a9543","year":2020},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"C.-M. Yoo, T. Harada, S. Hirano and K. Kohri,Abundance of Primordial Black Holes in Peak Theory for an Arbitrary Power Spectrum,PTEP2021(2021) 013E02 [2008.02425]","work_id":"4c46f2bf-ea75-404a-924c-5a2915cc5344","year":2021},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"M. Mirbabayi, A. Gruzinov and J. Nore˜ na,Spin of Primordial Black Holes,JCAP03(2020) 017 [1901.05963]","work_id":"a0e63472-e279-41e1-a985-97319b7f44c8","year":2020}],"snapshot_sha256":"f9bae1858219d225fa205626929b1ad4aea9eea85a117bd253d3216056f5398d"},"source":{"id":"2505.09202","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-22T15:58:24.965857Z","id":"4cb7013b-435f-47b9-a2fb-8f35c44c1329","model_set":{"reader":"grok-4.3"},"one_line_summary":"Computes the dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles from density and velocity perturbations in FOPTs, yielding values from O(10^{-5}) to O(10) and a scaling relation with FOPT timescale, wall velocity, and temperature ratio.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"False vacuum bubbles acquire dimensionless spins from 10^{-5} to 10 during dark-sector first-order phase transitions","strongest_claim":"The dimensionless spin parameter s = J/(G_N M^2) of false vacuum bubbles of mass M and angular momentum J take a wide range of values from O(10^{-5}) to O(10) for FOPTs between 10 keV and 100 GeV and a dark sector that is 0.1 to 0.4 times cooler than the visible sector. A scaling relation exists between the root-mean-square value of the spin, the FOPT time scale, the bubble wall velocity, and the dark sector-to-visible sector temperature ratio.","weakest_assumption":"Angular momentum of the bubbles is given exactly by the product of density and velocity perturbations, with bubbles remaining spherical while background quantities and transfer functions are tracked through the FOPT; this modeling choice is stated as the basis for the calculation in the abstract."}},"verdict_id":"4cb7013b-435f-47b9-a2fb-8f35c44c1329"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:770989b4d2686dfbe4be9dfdfdcf945bfcc225afa9dd0dfaa9d63d2be1d556e2","target":"record","created_at":"2026-06-19T16:11:10Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"735ee71ead241328c19db8da58d6a9911996c6ddf281b5b017e006d7f4e9f6c3","cross_cats_sorted":["astro-ph.CO","hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-14T07:28:01Z","title_canon_sha256":"9d9b845bfc155c51514bf5fc099be035dbaf29e3a87765d50aba8750afc54f97"},"schema_version":"1.0","source":{"id":"2505.09202","kind":"arxiv","version":3}},"canonical_sha256":"b514695418931c29901bd610252f59eabb0080fcb99674483c027e2e602f3794","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b514695418931c29901bd610252f59eabb0080fcb99674483c027e2e602f3794","first_computed_at":"2026-06-19T16:11:10.907115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-19T16:11:10.907115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sVqpTiH1qBVWfI79l+6b6I0JnCe1g8IwyO5hiuhJEHhlyTPMqFAeLg34HLY+NYOa+ep9MpvBmyBqM6bliNnaCA==","signature_status":"signed_v1","signed_at":"2026-06-19T16:11:10.907476Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.09202","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:770989b4d2686dfbe4be9dfdfdcf945bfcc225afa9dd0dfaa9d63d2be1d556e2","sha256:402ffb655e2d799c844ed2d4e42cb883c66536eb20b289b7ea60a2530f6e3a14"],"state_sha256":"fc8370f2508b4c24d80b9e7125620035bc859f6ee6d69359a14a5557a54b81c5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"INaFS4ul0Tcw3nx3/llxf7kDhLE/tY637tsKkuWCq1D3iUkB/SDcIQwHXZov/FRx6B5IOkk9I0GURtM9MPKkCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T01:21:51.547576Z","bundle_sha256":"d40271320d9bdc83e15a79470dfcdf561880c012689e4f83cbe2858ff8e488d7"}}