{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:POM4SEFVT4Z6BOPVU2TO3IG6SX","short_pith_number":"pith:POM4SEFV","schema_version":"1.0","canonical_sha256":"7b99c910b59f33e0b9f5a6a6eda0de95c1ab4e0e4843c50282e1d0fe1a37255c","source":{"kind":"arxiv","id":"2502.10135","version":2},"attestation_state":"computed","paper":{"title":"C-parity, magnetic monopoles and higher frequency gravitational waves","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":"2025-02-14T13:04:41Z","abstract_excerpt":"We consider the spontaneous breaking of $SO(10)$ grand unified symmetry to the left-right symmetric model $SU(3)_c \\times SU(3)_L \\times SU(2)_R \\times U(1)_{B-L}$ with C-parity also unbroken [$C$ converts $Q\\to -Q$, where $Q$ is the electric charge operator in $SO(10)$.] This breaking produces the topologically stable GUT monopole as well as a GUT scale C-string. The subsequent breaking at an intermediate scale of C-parity produces domain walls bounded by C-strings, found by Kibble, Lazarides and Shafi. A limited number of inflationary $e$-foldings experienced during these breakings can yield"},"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":"2502.10135","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-14T13:04:41Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"bf62efa92813c80ad22a14c01d3e6163e920201f50c4342bea994d2cf3a9522d","abstract_canon_sha256":"853a0465d1bb38265c6a6b25d2866da437ea351083249430e8ccfce5e29ed8a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:55:30.769651Z","signature_b64":"7KqW1OWzXfBENTqiX6YjIbFT2wNbWjJ2qytmUOOBl/ziwBlK2QpKkMQy/i7KvN8iPWka47CtzCPH0ynz1yLPBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b99c910b59f33e0b9f5a6a6eda0de95c1ab4e0e4843c50282e1d0fe1a37255c","last_reissued_at":"2026-07-05T10:55:30.769165Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:55:30.769165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"C-parity, magnetic monopoles and higher frequency gravitational waves","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":"2025-02-14T13:04:41Z","abstract_excerpt":"We consider the spontaneous breaking of $SO(10)$ grand unified symmetry to the left-right symmetric model $SU(3)_c \\times SU(3)_L \\times SU(2)_R \\times U(1)_{B-L}$ with C-parity also unbroken [$C$ converts $Q\\to -Q$, where $Q$ is the electric charge operator in $SO(10)$.] This breaking produces the topologically stable GUT monopole as well as a GUT scale C-string. The subsequent breaking at an intermediate scale of C-parity produces domain walls bounded by C-strings, found by Kibble, Lazarides and Shafi. A limited number of inflationary $e$-foldings experienced during these breakings can yield"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.10135","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/2502.10135/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":"2502.10135","created_at":"2026-07-05T10:55:30.769215+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.10135v2","created_at":"2026-07-05T10:55:30.769215+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.10135","created_at":"2026-07-05T10:55:30.769215+00:00"},{"alias_kind":"pith_short_12","alias_value":"POM4SEFVT4Z6","created_at":"2026-07-05T10:55:30.769215+00:00"},{"alias_kind":"pith_short_16","alias_value":"POM4SEFVT4Z6BOPV","created_at":"2026-07-05T10:55:30.769215+00:00"},{"alias_kind":"pith_short_8","alias_value":"POM4SEFV","created_at":"2026-07-05T10:55:30.769215+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.14323","citing_title":"High-Quality Axion Dark Matter at Gravitational Wave Interferometers","ref_index":103,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX","json":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX.json","graph_json":"https://pith.science/api/pith-number/POM4SEFVT4Z6BOPVU2TO3IG6SX/graph.json","events_json":"https://pith.science/api/pith-number/POM4SEFVT4Z6BOPVU2TO3IG6SX/events.json","paper":"https://pith.science/paper/POM4SEFV"},"agent_actions":{"view_html":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX","download_json":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX.json","view_paper":"https://pith.science/paper/POM4SEFV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.10135&json=true","fetch_graph":"https://pith.science/api/pith-number/POM4SEFVT4Z6BOPVU2TO3IG6SX/graph.json","fetch_events":"https://pith.science/api/pith-number/POM4SEFVT4Z6BOPVU2TO3IG6SX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX/action/storage_attestation","attest_author":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX/action/author_attestation","sign_citation":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX/action/citation_signature","submit_replication":"https://pith.science/pith/POM4SEFVT4Z6BOPVU2TO3IG6SX/action/replication_record"}},"created_at":"2026-07-05T10:55:30.769215+00:00","updated_at":"2026-07-05T10:55:30.769215+00:00"}