{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:ZD36KADP3V3D477WLKECW3HZ3V","short_pith_number":"pith:ZD36KADP","schema_version":"1.0","canonical_sha256":"c8f7e5006fdd763e7ff65a882b6cf9dd484479fcc07668aa2d7bd84b7d853af9","source":{"kind":"arxiv","id":"2105.12135","version":2},"attestation_state":"computed","paper":{"title":"Gravitational Wave Echo of Relaxion Trapping","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Abhishek Banerjee, Eric Madge, Gilad Perez, Pedro Schwaller, Wolfram Ratzinger","submitted_at":"2021-05-25T18:00:01Z","abstract_excerpt":"To solve the hierarchy problem, the relaxion must remain trapped in the correct minimum, even if the electroweak symmetry is restored after reheating. In this scenario, the relaxion starts rolling again until the backreaction potential, with its set of local minima, reappears. Depending on the time of barrier reappearance, Hubble friction alone may be insufficient to retrap the relaxion in a large portion of the parameter space. Thus, an additional source of friction is required, which might be provided by coupling to a dark photon.The dark photon experiences a tachyonic instability as the rel"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2105.12135","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-05-25T18:00:01Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"b15b61f566eff329ee85c76687c798291b1e0037d2631339af1f1a5960ce9dea","abstract_canon_sha256":"7a303865008cbc68d4acfbf937378059835ad3b8d8b9d1213c139eb3b4594215"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:18:17.553402Z","signature_b64":"f7zGIMPiHsWB8vPI6OSI4V1Q3537cvu4nptemPMZVC0FeZdvsITR77W7Y4ZSpK1ymvXp5x7OsMNPgx7d/ziGAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c8f7e5006fdd763e7ff65a882b6cf9dd484479fcc07668aa2d7bd84b7d853af9","last_reissued_at":"2026-07-05T03:18:17.552913Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:18:17.552913Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational Wave Echo of Relaxion Trapping","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Abhishek Banerjee, Eric Madge, Gilad Perez, Pedro Schwaller, Wolfram Ratzinger","submitted_at":"2021-05-25T18:00:01Z","abstract_excerpt":"To solve the hierarchy problem, the relaxion must remain trapped in the correct minimum, even if the electroweak symmetry is restored after reheating. In this scenario, the relaxion starts rolling again until the backreaction potential, with its set of local minima, reappears. Depending on the time of barrier reappearance, Hubble friction alone may be insufficient to retrap the relaxion in a large portion of the parameter space. Thus, an additional source of friction is required, which might be provided by coupling to a dark photon.The dark photon experiences a tachyonic instability as the rel"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.12135","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2105.12135/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2105.12135","created_at":"2026-07-05T03:18:17.552972+00:00"},{"alias_kind":"arxiv_version","alias_value":"2105.12135v2","created_at":"2026-07-05T03:18:17.552972+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.12135","created_at":"2026-07-05T03:18:17.552972+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZD36KADP3V3D","created_at":"2026-07-05T03:18:17.552972+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZD36KADP3V3D477W","created_at":"2026-07-05T03:18:17.552972+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZD36KADP","created_at":"2026-07-05T03:18:17.552972+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.21092","citing_title":"Audible Axion Magnetogenesis: Linking Intergalactic Magnetic Fields and Gravitational Waves","ref_index":31,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V","json":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V.json","graph_json":"https://pith.science/api/pith-number/ZD36KADP3V3D477WLKECW3HZ3V/graph.json","events_json":"https://pith.science/api/pith-number/ZD36KADP3V3D477WLKECW3HZ3V/events.json","paper":"https://pith.science/paper/ZD36KADP"},"agent_actions":{"view_html":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V","download_json":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V.json","view_paper":"https://pith.science/paper/ZD36KADP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2105.12135&json=true","fetch_graph":"https://pith.science/api/pith-number/ZD36KADP3V3D477WLKECW3HZ3V/graph.json","fetch_events":"https://pith.science/api/pith-number/ZD36KADP3V3D477WLKECW3HZ3V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V/action/storage_attestation","attest_author":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V/action/author_attestation","sign_citation":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V/action/citation_signature","submit_replication":"https://pith.science/pith/ZD36KADP3V3D477WLKECW3HZ3V/action/replication_record"}},"created_at":"2026-07-05T03:18:17.552972+00:00","updated_at":"2026-07-05T03:18:17.552972+00:00"}