{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:IHDLGY56BZC6QJ4IJGER3ED4YP","short_pith_number":"pith:IHDLGY56","canonical_record":{"source":{"id":"1009.2093","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-10T20:10:23Z","cross_cats_sorted":["astro-ph.CO","hep-ph"],"title_canon_sha256":"728c20507eb2efcdf0f372bb9b3bb784b4bea30aba98f2cfae13ba7c6ff320d5","abstract_canon_sha256":"56e4a624317ebb99a21837c1ea8f69293a1749525e8857dde5ba14e3ba99a63e"},"schema_version":"1.0"},"canonical_sha256":"41c6b363be0e45e8278849891d907cc3e590f29544e69b941509048526b64f66","source":{"kind":"arxiv","id":"1009.2093","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.2093","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"arxiv_version","alias_value":"1009.2093v2","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.2093","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"pith_short_12","alias_value":"IHDLGY56BZC6","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"IHDLGY56BZC6QJ4I","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"IHDLGY56","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:IHDLGY56BZC6QJ4IJGER3ED4YP","target":"record","payload":{"canonical_record":{"source":{"id":"1009.2093","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-10T20:10:23Z","cross_cats_sorted":["astro-ph.CO","hep-ph"],"title_canon_sha256":"728c20507eb2efcdf0f372bb9b3bb784b4bea30aba98f2cfae13ba7c6ff320d5","abstract_canon_sha256":"56e4a624317ebb99a21837c1ea8f69293a1749525e8857dde5ba14e3ba99a63e"},"schema_version":"1.0"},"canonical_sha256":"41c6b363be0e45e8278849891d907cc3e590f29544e69b941509048526b64f66","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:05:31.812022Z","signature_b64":"AhQNF4lLZiSGFdUQzeC/rHdQlgpJciZiwvlUKu20KRU2YJjc6HEQd/BiDt7cs+9OegsCVljHZCDVsgArpt7WAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"41c6b363be0e45e8278849891d907cc3e590f29544e69b941509048526b64f66","last_reissued_at":"2026-05-18T02:05:31.811162Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:05:31.811162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1009.2093","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:05:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NGzLCsKTC4i9iguCFr5jpFxcTKx+ScmcLRZf0GM0AxR8ew635ay4A5BckCDLmDrXSYcgZDHveEUGCjdn7KoVCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T09:03:09.127169Z"},"content_sha256":"b3e3062ec7382c4d6b062844e960796a1663285317d8c952815e56e1bb4b9dfb","schema_version":"1.0","event_id":"sha256:b3e3062ec7382c4d6b062844e960796a1663285317d8c952815e56e1bb4b9dfb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:IHDLGY56BZC6QJ4IJGER3ED4YP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Effective Field Theory of Multifield Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph"],"primary_cat":"hep-th","authors_text":"Leonardo Senatore, Matias Zaldarriaga","submitted_at":"2010-09-10T20:10:23Z","abstract_excerpt":"We generalize the Effective Field Theory of Inflation to include additional light scalar degrees of freedom that are in their vacuum at the time the modes of interest are crossing the horizon. In order to make the scalars light in a natural way we consider the case where they are the Goldstone bosons of a global symmetry group or are partially protected by an approximate supersymmetry. We write the most general Lagrangian that couples the scalar mode associated to the breaking of time translation during inflation to the additional light scalar fields. This Lagrangian is constrained by diffeomo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.2093","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":""},"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":"2026-05-18T02:05:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VA64l06aKdvXHaUJO1juInWRSUWO3EB0R+oE/jtPAGiXfnXbNrCgCmC5XXYCBsMgveWIuTeSStelzkIVV4sqAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T09:03:09.127851Z"},"content_sha256":"b96d1f244456592b8018a232bb900dcab09de1cd1ea4fc7698d362ce999b074d","schema_version":"1.0","event_id":"sha256:b96d1f244456592b8018a232bb900dcab09de1cd1ea4fc7698d362ce999b074d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/bundle.json","state_url":"https://pith.science/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/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":"2026-06-10T09:03:09Z","links":{"resolver":"https://pith.science/pith/IHDLGY56BZC6QJ4IJGER3ED4YP","bundle":"https://pith.science/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/bundle.json","state":"https://pith.science/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IHDLGY56BZC6QJ4IJGER3ED4YP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:IHDLGY56BZC6QJ4IJGER3ED4YP","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":"56e4a624317ebb99a21837c1ea8f69293a1749525e8857dde5ba14e3ba99a63e","cross_cats_sorted":["astro-ph.CO","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-10T20:10:23Z","title_canon_sha256":"728c20507eb2efcdf0f372bb9b3bb784b4bea30aba98f2cfae13ba7c6ff320d5"},"schema_version":"1.0","source":{"id":"1009.2093","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.2093","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"arxiv_version","alias_value":"1009.2093v2","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.2093","created_at":"2026-05-18T02:05:31Z"},{"alias_kind":"pith_short_12","alias_value":"IHDLGY56BZC6","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"IHDLGY56BZC6QJ4I","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"IHDLGY56","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:b96d1f244456592b8018a232bb900dcab09de1cd1ea4fc7698d362ce999b074d","target":"graph","created_at":"2026-05-18T02:05:31Z","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 generalize the Effective Field Theory of Inflation to include additional light scalar degrees of freedom that are in their vacuum at the time the modes of interest are crossing the horizon. In order to make the scalars light in a natural way we consider the case where they are the Goldstone bosons of a global symmetry group or are partially protected by an approximate supersymmetry. We write the most general Lagrangian that couples the scalar mode associated to the breaking of time translation during inflation to the additional light scalar fields. This Lagrangian is constrained by diffeomo","authors_text":"Leonardo Senatore, Matias Zaldarriaga","cross_cats":["astro-ph.CO","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-10T20:10:23Z","title":"The Effective Field Theory of Multifield Inflation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.2093","kind":"arxiv","version":2},"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:b3e3062ec7382c4d6b062844e960796a1663285317d8c952815e56e1bb4b9dfb","target":"record","created_at":"2026-05-18T02:05:31Z","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":"56e4a624317ebb99a21837c1ea8f69293a1749525e8857dde5ba14e3ba99a63e","cross_cats_sorted":["astro-ph.CO","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-09-10T20:10:23Z","title_canon_sha256":"728c20507eb2efcdf0f372bb9b3bb784b4bea30aba98f2cfae13ba7c6ff320d5"},"schema_version":"1.0","source":{"id":"1009.2093","kind":"arxiv","version":2}},"canonical_sha256":"41c6b363be0e45e8278849891d907cc3e590f29544e69b941509048526b64f66","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"41c6b363be0e45e8278849891d907cc3e590f29544e69b941509048526b64f66","first_computed_at":"2026-05-18T02:05:31.811162Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:05:31.811162Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AhQNF4lLZiSGFdUQzeC/rHdQlgpJciZiwvlUKu20KRU2YJjc6HEQd/BiDt7cs+9OegsCVljHZCDVsgArpt7WAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:05:31.812022Z","signed_message":"canonical_sha256_bytes"},"source_id":"1009.2093","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b3e3062ec7382c4d6b062844e960796a1663285317d8c952815e56e1bb4b9dfb","sha256:b96d1f244456592b8018a232bb900dcab09de1cd1ea4fc7698d362ce999b074d"],"state_sha256":"e9f639890866f9c305881c75fabd0a47bdbd019b7fa525c6c09fc6a6c5825a87"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UbxFEWnNNtaeGLti+IX1knGRqk2J/eIyMSm8RU83kexjnnZeOkRYwM2OtvTMiaorrl8nEOpRdPPZlq6PN5UWCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T09:03:09.132067Z","bundle_sha256":"fef4a11b384da3eb04f148e52304b353da3feadb810dc3e0e8a8fe6a4ad66bd8"}}