{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:ZWATRZ7XBNWNK2SXQTLU66RSFP","short_pith_number":"pith:ZWATRZ7X","canonical_record":{"source":{"id":"2308.00395","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-01T09:15:56Z","cross_cats_sorted":[],"title_canon_sha256":"e79db6a72b585109ffd39c09ff2c7a3a462c8adf7f550221ff467bb9d9d61193","abstract_canon_sha256":"fcd7568092156950969eeb08b9471dd2be7a6c22fa39492d6f8ace87615f698c"},"schema_version":"1.0"},"canonical_sha256":"cd8138e7f70b6cd56a5784d74f7a322bf6cd82b25b312449055a84b5ae5d1481","source":{"kind":"arxiv","id":"2308.00395","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2308.00395","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"arxiv_version","alias_value":"2308.00395v3","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2308.00395","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_12","alias_value":"ZWATRZ7XBNWN","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_16","alias_value":"ZWATRZ7XBNWNK2SX","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_8","alias_value":"ZWATRZ7X","created_at":"2026-07-05T08:17:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:ZWATRZ7XBNWNK2SXQTLU66RSFP","target":"record","payload":{"canonical_record":{"source":{"id":"2308.00395","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-01T09:15:56Z","cross_cats_sorted":[],"title_canon_sha256":"e79db6a72b585109ffd39c09ff2c7a3a462c8adf7f550221ff467bb9d9d61193","abstract_canon_sha256":"fcd7568092156950969eeb08b9471dd2be7a6c22fa39492d6f8ace87615f698c"},"schema_version":"1.0"},"canonical_sha256":"cd8138e7f70b6cd56a5784d74f7a322bf6cd82b25b312449055a84b5ae5d1481","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:17:58.615842Z","signature_b64":"FmtXzVBNRUq9+74mHVtOaO7Fv4qE4obEcS3xMKdOwayDwPetoDfIzijJFKibcxUdqBEVnlTNcmqDoKmNncXJCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cd8138e7f70b6cd56a5784d74f7a322bf6cd82b25b312449055a84b5ae5d1481","last_reissued_at":"2026-07-05T08:17:58.615364Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:17:58.615364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2308.00395","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":"2026-07-05T08:17:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pHiuOsx7QB+lKIpw6xBfLnYGZHNOeAnxqeFAwBNX8AehNOtCuN6blUniuDzbskq1eBW8B1SFsGle4Dl3+TXNBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T06:07:40.096179Z"},"content_sha256":"260c9f2e39132f3651d2c878db997e0092d9bcc00af2b0ed588b9aaf5858ed09","schema_version":"1.0","event_id":"sha256:260c9f2e39132f3651d2c878db997e0092d9bcc00af2b0ed588b9aaf5858ed09"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:ZWATRZ7XBNWNK2SXQTLU66RSFP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gravitational wave effects and phenomenology of a two-component dark matter model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ahmad Mohamadnejad, Mojtaba Hosseini, Seyed Yaser Ayazi","submitted_at":"2023-08-01T09:15:56Z","abstract_excerpt":"We study an extension of the Standard Model (SM) which could have two candidates for dark matter (DM) including a Dirac fermion and a vector dark matter (VDM) under a new $U(1)$ gauge group in the hidden sector. The model is classically scale-invariant and the electroweak symmetry breaks because of loop effects. We investigate the parameter space allowed by current experimental constraints and phenomenological bounds. We probe the parameter space of the model in the mass range $1< M_V<5000$ GeV and $1<M_{\\psi}<5000$ GeV. It has been shown that there are many points in this mass range that are "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2308.00395","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/2308.00395/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":"2026-07-05T08:17:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/E0MpcYRnpGt01z0dodn2VpZAPHKkohAcPOU2v1wwWmGSeldp34rzV/3fyFlcXiv7IQ1FsbnOMiQOyAaoFamAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T06:07:40.096763Z"},"content_sha256":"e47243d5f9fa698b0d4923aeda0ad53513a0a0b22f4f87c4acf9f5f4a706b50e","schema_version":"1.0","event_id":"sha256:e47243d5f9fa698b0d4923aeda0ad53513a0a0b22f4f87c4acf9f5f4a706b50e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/bundle.json","state_url":"https://pith.science/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/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":"2026-08-16T06:07:40Z","links":{"resolver":"https://pith.science/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP","bundle":"https://pith.science/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/bundle.json","state":"https://pith.science/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZWATRZ7XBNWNK2SXQTLU66RSFP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:ZWATRZ7XBNWNK2SXQTLU66RSFP","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":"fcd7568092156950969eeb08b9471dd2be7a6c22fa39492d6f8ace87615f698c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-01T09:15:56Z","title_canon_sha256":"e79db6a72b585109ffd39c09ff2c7a3a462c8adf7f550221ff467bb9d9d61193"},"schema_version":"1.0","source":{"id":"2308.00395","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2308.00395","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"arxiv_version","alias_value":"2308.00395v3","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2308.00395","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_12","alias_value":"ZWATRZ7XBNWN","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_16","alias_value":"ZWATRZ7XBNWNK2SX","created_at":"2026-07-05T08:17:58Z"},{"alias_kind":"pith_short_8","alias_value":"ZWATRZ7X","created_at":"2026-07-05T08:17:58Z"}],"graph_snapshots":[{"event_id":"sha256:e47243d5f9fa698b0d4923aeda0ad53513a0a0b22f4f87c4acf9f5f4a706b50e","target":"graph","created_at":"2026-07-05T08:17:58Z","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/2308.00395/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study an extension of the Standard Model (SM) which could have two candidates for dark matter (DM) including a Dirac fermion and a vector dark matter (VDM) under a new $U(1)$ gauge group in the hidden sector. The model is classically scale-invariant and the electroweak symmetry breaks because of loop effects. We investigate the parameter space allowed by current experimental constraints and phenomenological bounds. We probe the parameter space of the model in the mass range $1< M_V<5000$ GeV and $1<M_{\\psi}<5000$ GeV. It has been shown that there are many points in this mass range that are ","authors_text":"Ahmad Mohamadnejad, Mojtaba Hosseini, Seyed Yaser Ayazi","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-01T09:15:56Z","title":"Gravitational wave effects and phenomenology of a two-component dark matter model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2308.00395","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":"sha256:260c9f2e39132f3651d2c878db997e0092d9bcc00af2b0ed588b9aaf5858ed09","target":"record","created_at":"2026-07-05T08:17:58Z","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":"fcd7568092156950969eeb08b9471dd2be7a6c22fa39492d6f8ace87615f698c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-08-01T09:15:56Z","title_canon_sha256":"e79db6a72b585109ffd39c09ff2c7a3a462c8adf7f550221ff467bb9d9d61193"},"schema_version":"1.0","source":{"id":"2308.00395","kind":"arxiv","version":3}},"canonical_sha256":"cd8138e7f70b6cd56a5784d74f7a322bf6cd82b25b312449055a84b5ae5d1481","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cd8138e7f70b6cd56a5784d74f7a322bf6cd82b25b312449055a84b5ae5d1481","first_computed_at":"2026-07-05T08:17:58.615364Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:17:58.615364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FmtXzVBNRUq9+74mHVtOaO7Fv4qE4obEcS3xMKdOwayDwPetoDfIzijJFKibcxUdqBEVnlTNcmqDoKmNncXJCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:17:58.615842Z","signed_message":"canonical_sha256_bytes"},"source_id":"2308.00395","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:260c9f2e39132f3651d2c878db997e0092d9bcc00af2b0ed588b9aaf5858ed09","sha256:e47243d5f9fa698b0d4923aeda0ad53513a0a0b22f4f87c4acf9f5f4a706b50e"],"state_sha256":"13b299ba7bc5723a58a027276188ef7026109b5a7c091c044428acc277cf68d2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VgM21ynBePyhaJNeaF8XyeFQDF7w5xeTQ5vLlTpcE82fd4IPS3ls1En/wPuRf6S+qZKD1SIkpaOJRaoM3m9GAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T06:07:40.102471Z","bundle_sha256":"cbb54a740e45f6a489c3fe7e71d6394d51f92cc11dd1676ec9b230b5ca3c581f"}}