{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6OV2QBUJ5X4ZWURPXBVVQLGY2F","short_pith_number":"pith:6OV2QBUJ","canonical_record":{"source":{"id":"1404.1450","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-05T09:17:31Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"b357079d1873a14e39c9619d896093e1e651b392a781810a478088ff0cd6432e","abstract_canon_sha256":"e85201ba807c0d144a2724609d304dac13398a06207b20240a0feb50635919ba"},"schema_version":"1.0"},"canonical_sha256":"f3aba80689edf99b522fb86b582cd8d15ae50d38cb09c63ad380359e4112c498","source":{"kind":"arxiv","id":"1404.1450","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.1450","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"arxiv_version","alias_value":"1404.1450v3","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.1450","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"pith_short_12","alias_value":"6OV2QBUJ5X4Z","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6OV2QBUJ5X4ZWURP","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6OV2QBUJ","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6OV2QBUJ5X4ZWURPXBVVQLGY2F","target":"record","payload":{"canonical_record":{"source":{"id":"1404.1450","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-05T09:17:31Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"b357079d1873a14e39c9619d896093e1e651b392a781810a478088ff0cd6432e","abstract_canon_sha256":"e85201ba807c0d144a2724609d304dac13398a06207b20240a0feb50635919ba"},"schema_version":"1.0"},"canonical_sha256":"f3aba80689edf99b522fb86b582cd8d15ae50d38cb09c63ad380359e4112c498","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:49:28.440557Z","signature_b64":"0ehy2JQEeDtExdsgZvaagZa2WzfaB1AcwUPCD1/xqRPT9MFSF4tDIN7oGII9dPQm+x8Cf33FqRnfg3DMPqvfBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f3aba80689edf99b522fb86b582cd8d15ae50d38cb09c63ad380359e4112c498","last_reissued_at":"2026-05-18T02:49:28.439875Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:49:28.439875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.1450","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":"2026-05-18T02:49:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eqOUjMb6mUYpAjsLl48VCJvzutaRPn+Be9QNoSxR7ZxHvNsYz75VncUeUyBd1HLwc2Jr/qR9zmFV2ox873v8BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:39:27.205667Z"},"content_sha256":"0be1e644e85ec8776e6236cd058d1501032a153e993b0f6ead0352260844673d","schema_version":"1.0","event_id":"sha256:0be1e644e85ec8776e6236cd058d1501032a153e993b0f6ead0352260844673d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6OV2QBUJ5X4ZWURPXBVVQLGY2F","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"TeV scale seesaw from supersymmetric Higgs-lepton inflation and BICEP2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Nobuchika Okada, Shinsuke Kawai","submitted_at":"2014-04-05T09:17:31Z","abstract_excerpt":"We discuss the physics resulting from the supersymmetric Higgs-lepton inflation model and the recent CMB B-mode observation by the BICEP2 experiment. The tensor-to-scalar ratio r=0.20+0.07-0.05 of the primordial fluctuations indicated by the CMB B-mode polarization is consistent with the prediction of this inflationary model for natural parameter values. A salient feature of the model is that it predicts the seesaw mass scale M from the amplitude of the tensor mode fluctuations. It is found that the 68% (95%) confidence level (CL) constraints from the BICEP2 experiment give 927 GeV < M < 1.62 "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.1450","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":""},"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":"2026-05-18T02:49:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2bc3nv8wES4E8GvWnmN75eyPTJwqcLVj7/Yhwvj1fXwo/Fa7LCQAZ928WRqeBvbiz9nlyBWLhPBGDuOxmQ3GDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T11:39:27.206356Z"},"content_sha256":"f9f74a602773a44a62b16258c19893fcacd57dd61722b8059ff721b28be7649a","schema_version":"1.0","event_id":"sha256:f9f74a602773a44a62b16258c19893fcacd57dd61722b8059ff721b28be7649a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/bundle.json","state_url":"https://pith.science/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/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":"2026-05-27T11:39:27Z","links":{"resolver":"https://pith.science/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F","bundle":"https://pith.science/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/bundle.json","state":"https://pith.science/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6OV2QBUJ5X4ZWURPXBVVQLGY2F/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6OV2QBUJ5X4ZWURPXBVVQLGY2F","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":"e85201ba807c0d144a2724609d304dac13398a06207b20240a0feb50635919ba","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-05T09:17:31Z","title_canon_sha256":"b357079d1873a14e39c9619d896093e1e651b392a781810a478088ff0cd6432e"},"schema_version":"1.0","source":{"id":"1404.1450","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.1450","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"arxiv_version","alias_value":"1404.1450v3","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.1450","created_at":"2026-05-18T02:49:28Z"},{"alias_kind":"pith_short_12","alias_value":"6OV2QBUJ5X4Z","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6OV2QBUJ5X4ZWURP","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6OV2QBUJ","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:f9f74a602773a44a62b16258c19893fcacd57dd61722b8059ff721b28be7649a","target":"graph","created_at":"2026-05-18T02:49:28Z","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"},"paper":{"abstract_excerpt":"We discuss the physics resulting from the supersymmetric Higgs-lepton inflation model and the recent CMB B-mode observation by the BICEP2 experiment. The tensor-to-scalar ratio r=0.20+0.07-0.05 of the primordial fluctuations indicated by the CMB B-mode polarization is consistent with the prediction of this inflationary model for natural parameter values. A salient feature of the model is that it predicts the seesaw mass scale M from the amplitude of the tensor mode fluctuations. It is found that the 68% (95%) confidence level (CL) constraints from the BICEP2 experiment give 927 GeV < M < 1.62 ","authors_text":"Nobuchika Okada, Shinsuke Kawai","cross_cats":["astro-ph.CO","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-05T09:17:31Z","title":"TeV scale seesaw from supersymmetric Higgs-lepton inflation and BICEP2"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.1450","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":"sha256:0be1e644e85ec8776e6236cd058d1501032a153e993b0f6ead0352260844673d","target":"record","created_at":"2026-05-18T02:49:28Z","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":"e85201ba807c0d144a2724609d304dac13398a06207b20240a0feb50635919ba","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-05T09:17:31Z","title_canon_sha256":"b357079d1873a14e39c9619d896093e1e651b392a781810a478088ff0cd6432e"},"schema_version":"1.0","source":{"id":"1404.1450","kind":"arxiv","version":3}},"canonical_sha256":"f3aba80689edf99b522fb86b582cd8d15ae50d38cb09c63ad380359e4112c498","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f3aba80689edf99b522fb86b582cd8d15ae50d38cb09c63ad380359e4112c498","first_computed_at":"2026-05-18T02:49:28.439875Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:49:28.439875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0ehy2JQEeDtExdsgZvaagZa2WzfaB1AcwUPCD1/xqRPT9MFSF4tDIN7oGII9dPQm+x8Cf33FqRnfg3DMPqvfBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:49:28.440557Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.1450","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0be1e644e85ec8776e6236cd058d1501032a153e993b0f6ead0352260844673d","sha256:f9f74a602773a44a62b16258c19893fcacd57dd61722b8059ff721b28be7649a"],"state_sha256":"f2f7a99aa737c0d7f937ed365ab1150a98b7b784bbcc772533ab757c14a1271c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g+ByJVdnL5bV0UrUZzIV8kLBIqrFtI7jugMpXG4dQtO1MyoNdvvqo5XVU5BMz338CHdQGDwbVNWVQN/SJvxaBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T11:39:27.209012Z","bundle_sha256":"2a6c22ef6932635c9a73db44d82d6e15a74dda311dfeabd707b5f06d13a4a0e1"}}