{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:HRX7KJONSVC6OMJSJHP6QMZCMN","short_pith_number":"pith:HRX7KJON","canonical_record":{"source":{"id":"2112.14483","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-29T10:01:40Z","cross_cats_sorted":[],"title_canon_sha256":"2355de21dd178fc725dff413002398fe18f484d32465fcbb110efe2c1e5594c7","abstract_canon_sha256":"c2ae3eeae4f78cec108b30cdd9bc390c4b24d7beceb58e5ecae497c26447904a"},"schema_version":"1.0"},"canonical_sha256":"3c6ff525cd9545e7313249dfe833226361ac34893ed9ebfe7ee2862e19957d4c","source":{"kind":"arxiv","id":"2112.14483","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2112.14483","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"arxiv_version","alias_value":"2112.14483v3","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.14483","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_12","alias_value":"HRX7KJONSVC6","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_16","alias_value":"HRX7KJONSVC6OMJS","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_8","alias_value":"HRX7KJON","created_at":"2026-07-05T04:52:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:HRX7KJONSVC6OMJSJHP6QMZCMN","target":"record","payload":{"canonical_record":{"source":{"id":"2112.14483","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-29T10:01:40Z","cross_cats_sorted":[],"title_canon_sha256":"2355de21dd178fc725dff413002398fe18f484d32465fcbb110efe2c1e5594c7","abstract_canon_sha256":"c2ae3eeae4f78cec108b30cdd9bc390c4b24d7beceb58e5ecae497c26447904a"},"schema_version":"1.0"},"canonical_sha256":"3c6ff525cd9545e7313249dfe833226361ac34893ed9ebfe7ee2862e19957d4c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:52:46.914347Z","signature_b64":"OlBcqxlU9PlwJV1gacza7mZtMxGr970rIHHqSuuPimjqzbB+Uxd9pJ6gq/Xg/C6IdVwxLB/Vkr8X5q4is43jAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c6ff525cd9545e7313249dfe833226361ac34893ed9ebfe7ee2862e19957d4c","last_reissued_at":"2026-07-05T04:52:46.913877Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:52:46.913877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2112.14483","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":"2026-07-05T04:52:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"167mBtbfCRdR4wD7iul4z5Gh8l/ImAra+mv+bqOnhcrx7UdOKnF4Jy9JrTH1MvuYHFsb80qmoyaE/eoHR1awBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-23T09:11:29.819848Z"},"content_sha256":"13a6ccaa39480b11c8d9c577113cff5dae3254313b5f7f3bc3a99f4169221afb","schema_version":"1.0","event_id":"sha256:13a6ccaa39480b11c8d9c577113cff5dae3254313b5f7f3bc3a99f4169221afb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:HRX7KJONSVC6OMJSJHP6QMZCMN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tracking Down the Route to the SM with Inflation and Gravitational Waves","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Eung Jin Chun, Liliana Velasco-Sevilla","submitted_at":"2021-12-29T10:01:40Z","abstract_excerpt":"We explore supersymmetric SO(10) models predicting observable proton decay and various topological defects which produce different shapes and strengths of gravitational wave backgrounds depending on the scales of intermediate symmetry breaking and inflation as well. We compare these to their non-supersymmetric counterparts. By identifying the scales at which gravitational wave signals appear, we would be able to track down a particular breaking chain and discern if it has a supersymmetric origin or not. It would also be useful to observe gravitational waves from more than one source among all "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.14483","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/2112.14483/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T04:52:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CpczFdh43JvLAZa+0qlnyBdUNi6+q91JudIKoRDimcyRx1WJVq/06Kh908NAv2h4AbFGPZuD5FBHPrUoZb+6CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-23T09:11:29.820211Z"},"content_sha256":"ed104ea90b42971c810a7f3656b371a2cfb94279d231075afd6135d1d5c95244","schema_version":"1.0","event_id":"sha256:ed104ea90b42971c810a7f3656b371a2cfb94279d231075afd6135d1d5c95244"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/bundle.json","state_url":"https://pith.science/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/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":"2026-07-23T09:11:29Z","links":{"resolver":"https://pith.science/pith/HRX7KJONSVC6OMJSJHP6QMZCMN","bundle":"https://pith.science/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/bundle.json","state":"https://pith.science/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HRX7KJONSVC6OMJSJHP6QMZCMN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:HRX7KJONSVC6OMJSJHP6QMZCMN","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":"c2ae3eeae4f78cec108b30cdd9bc390c4b24d7beceb58e5ecae497c26447904a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-29T10:01:40Z","title_canon_sha256":"2355de21dd178fc725dff413002398fe18f484d32465fcbb110efe2c1e5594c7"},"schema_version":"1.0","source":{"id":"2112.14483","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2112.14483","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"arxiv_version","alias_value":"2112.14483v3","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.14483","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_12","alias_value":"HRX7KJONSVC6","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_16","alias_value":"HRX7KJONSVC6OMJS","created_at":"2026-07-05T04:52:46Z"},{"alias_kind":"pith_short_8","alias_value":"HRX7KJON","created_at":"2026-07-05T04:52:46Z"}],"graph_snapshots":[{"event_id":"sha256:ed104ea90b42971c810a7f3656b371a2cfb94279d231075afd6135d1d5c95244","target":"graph","created_at":"2026-07-05T04:52:46Z","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":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2112.14483/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We explore supersymmetric SO(10) models predicting observable proton decay and various topological defects which produce different shapes and strengths of gravitational wave backgrounds depending on the scales of intermediate symmetry breaking and inflation as well. We compare these to their non-supersymmetric counterparts. By identifying the scales at which gravitational wave signals appear, we would be able to track down a particular breaking chain and discern if it has a supersymmetric origin or not. It would also be useful to observe gravitational waves from more than one source among all ","authors_text":"Eung Jin Chun, Liliana Velasco-Sevilla","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-29T10:01:40Z","title":"Tracking Down the Route to the SM with Inflation and Gravitational Waves"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.14483","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:13a6ccaa39480b11c8d9c577113cff5dae3254313b5f7f3bc3a99f4169221afb","target":"record","created_at":"2026-07-05T04:52:46Z","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":"c2ae3eeae4f78cec108b30cdd9bc390c4b24d7beceb58e5ecae497c26447904a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-12-29T10:01:40Z","title_canon_sha256":"2355de21dd178fc725dff413002398fe18f484d32465fcbb110efe2c1e5594c7"},"schema_version":"1.0","source":{"id":"2112.14483","kind":"arxiv","version":3}},"canonical_sha256":"3c6ff525cd9545e7313249dfe833226361ac34893ed9ebfe7ee2862e19957d4c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3c6ff525cd9545e7313249dfe833226361ac34893ed9ebfe7ee2862e19957d4c","first_computed_at":"2026-07-05T04:52:46.913877Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:52:46.913877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OlBcqxlU9PlwJV1gacza7mZtMxGr970rIHHqSuuPimjqzbB+Uxd9pJ6gq/Xg/C6IdVwxLB/Vkr8X5q4is43jAA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:52:46.914347Z","signed_message":"canonical_sha256_bytes"},"source_id":"2112.14483","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:13a6ccaa39480b11c8d9c577113cff5dae3254313b5f7f3bc3a99f4169221afb","sha256:ed104ea90b42971c810a7f3656b371a2cfb94279d231075afd6135d1d5c95244"],"state_sha256":"5c8c1fdbb98535b034fa12b7b18966c27cef01253c585890d1fff4bd16286d33"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"58TDY1jJYRjjKcBt1Da5uODCPXPkbA5HG9mFa69y4U8pb86O/ldqejcR2VNm5djB3AwjHX2Ci566XbkOB0cNCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-23T09:11:29.822563Z","bundle_sha256":"9d79aa17f99f3782fba06c4dc5b63eb54c327c7a4418c9c7862cc1bf56cd3529"}}