{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:53BMOE3T45MLVQ7VEHQBNEJX2F","short_pith_number":"pith:53BMOE3T","schema_version":"1.0","canonical_sha256":"eec2c71373e758bac3f521e0169137d1795c95d2a754e2f56466f84fbb268b54","source":{"kind":"arxiv","id":"2603.02996","version":3},"attestation_state":"computed","paper":{"title":"Magnetic monopoles and high frequency gravitational waves from quasi-stable strings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Qaisar Shafi, Rinku Maji","submitted_at":"2026-03-03T13:48:25Z","abstract_excerpt":"The spontaneous breaking of $SO(10)$ via flipped $SU(5)$ to the Standard Model yields a novel scenario in which the superheavy topologically stable GUT monopole carrying a single unit ($2\\pi/e$) of Dirac magnetic charge emerges from the merger of a confined but topologically distinct monopole-antimonopole pair that are pulled together by a string. The $SO(10)$ breaking via the subgroup $SU(4)_c\\times SU(2)_L\\times SU(2)_R$, following a similar reasoning, produces a topologically stable monopole that carries two units ($4\\pi/e$) of Dirac charge. We explore the cosmological consequences of this "},"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":"2603.02996","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-03T13:48:25Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"53e4f60ff2d92ee5ef825c238246d7bb913b4aef76feda274c427154c66a3eb1","abstract_canon_sha256":"14e03e57fcf08c7b37a900fcaaa2bf25f5757c4b1ed71270d53cbafa96886805"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-12T01:09:24.388475Z","signature_b64":"/+ayWUGmknXEIlMtNwimUjubSHjl/szvUQAhfW3w7nMIIIjiVwa5OKqA4ZwO7CHqUYrXdVKxg8OXZMrItE1CDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eec2c71373e758bac3f521e0169137d1795c95d2a754e2f56466f84fbb268b54","last_reissued_at":"2026-06-12T01:09:24.387894Z","signature_status":"signed_v1","first_computed_at":"2026-06-12T01:09:24.387894Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic monopoles and high frequency gravitational waves from quasi-stable strings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Qaisar Shafi, Rinku Maji","submitted_at":"2026-03-03T13:48:25Z","abstract_excerpt":"The spontaneous breaking of $SO(10)$ via flipped $SU(5)$ to the Standard Model yields a novel scenario in which the superheavy topologically stable GUT monopole carrying a single unit ($2\\pi/e$) of Dirac magnetic charge emerges from the merger of a confined but topologically distinct monopole-antimonopole pair that are pulled together by a string. The $SO(10)$ breaking via the subgroup $SU(4)_c\\times SU(2)_L\\times SU(2)_R$, following a similar reasoning, produces a topologically stable monopole that carries two units ($4\\pi/e$) of Dirac charge. We explore the cosmological consequences of this "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.02996","kind":"arxiv","version":3},"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/2603.02996/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":"2603.02996","created_at":"2026-06-12T01:09:24.387962+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.02996v3","created_at":"2026-06-12T01:09:24.387962+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.02996","created_at":"2026-06-12T01:09:24.387962+00:00"},{"alias_kind":"pith_short_12","alias_value":"53BMOE3T45ML","created_at":"2026-06-12T01:09:24.387962+00:00"},{"alias_kind":"pith_short_16","alias_value":"53BMOE3T45MLVQ7V","created_at":"2026-06-12T01:09:24.387962+00:00"},{"alias_kind":"pith_short_8","alias_value":"53BMOE3T","created_at":"2026-06-12T01:09:24.387962+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.28097","citing_title":"New gravitational-wave templates for metastable cosmic strings: Loop breaking versus network collapse","ref_index":68,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F","json":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F.json","graph_json":"https://pith.science/api/pith-number/53BMOE3T45MLVQ7VEHQBNEJX2F/graph.json","events_json":"https://pith.science/api/pith-number/53BMOE3T45MLVQ7VEHQBNEJX2F/events.json","paper":"https://pith.science/paper/53BMOE3T"},"agent_actions":{"view_html":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F","download_json":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F.json","view_paper":"https://pith.science/paper/53BMOE3T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.02996&json=true","fetch_graph":"https://pith.science/api/pith-number/53BMOE3T45MLVQ7VEHQBNEJX2F/graph.json","fetch_events":"https://pith.science/api/pith-number/53BMOE3T45MLVQ7VEHQBNEJX2F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F/action/storage_attestation","attest_author":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F/action/author_attestation","sign_citation":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F/action/citation_signature","submit_replication":"https://pith.science/pith/53BMOE3T45MLVQ7VEHQBNEJX2F/action/replication_record"}},"created_at":"2026-06-12T01:09:24.387962+00:00","updated_at":"2026-06-12T01:09:24.387962+00:00"}