{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:6CE6QSAZSSW3WQBVI4BCLP627G","short_pith_number":"pith:6CE6QSAZ","canonical_record":{"source":{"id":"1010.5495","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-10-26T19:29:35Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"3e41f6039c03ad7b2851459661f660de6151b72cb2d32cab296575b33bfa022a","abstract_canon_sha256":"6df72425b581d55909f89c6332d0ab44d041d000c35b43293973d262b309a2e5"},"schema_version":"1.0"},"canonical_sha256":"f089e8481994adbb4035470225bfdaf998b29388930c612ea8c5e11f93b23a23","source":{"kind":"arxiv","id":"1010.5495","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.5495","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"arxiv_version","alias_value":"1010.5495v2","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.5495","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"pith_short_12","alias_value":"6CE6QSAZSSW3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6CE6QSAZSSW3WQBV","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6CE6QSAZ","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:6CE6QSAZSSW3WQBVI4BCLP627G","target":"record","payload":{"canonical_record":{"source":{"id":"1010.5495","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-10-26T19:29:35Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"3e41f6039c03ad7b2851459661f660de6151b72cb2d32cab296575b33bfa022a","abstract_canon_sha256":"6df72425b581d55909f89c6332d0ab44d041d000c35b43293973d262b309a2e5"},"schema_version":"1.0"},"canonical_sha256":"f089e8481994adbb4035470225bfdaf998b29388930c612ea8c5e11f93b23a23","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:29.337660Z","signature_b64":"TcEGYEiBGSHgGKryMeCLnTaesmcPMKhiYGN9NYIeZa+5CKp6KG4oTqLonF8+fhs0NB0G4gLBlJCl3kx55O1RAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f089e8481994adbb4035470225bfdaf998b29388930c612ea8c5e11f93b23a23","last_reissued_at":"2026-05-18T04:28:29.337300Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:29.337300Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.5495","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":"2026-05-18T04:28:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oL66z5yMXWF87nIUKwGcgMzVamNi2iET3GrT1UR1b4ilO8CKtHy32wQNDD4HP6sJLzeVS7KSVRMGnbFr5SOsCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T11:51:12.963038Z"},"content_sha256":"19fe37402a20e27dbdd6a1c6d44416eaaba75e9efa0b8dc031c2db5c7ef1b538","schema_version":"1.0","event_id":"sha256:19fe37402a20e27dbdd6a1c6d44416eaaba75e9efa0b8dc031c2db5c7ef1b538"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:6CE6QSAZSSW3WQBVI4BCLP627G","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anisotropic Inflation from Charged Scalar Fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Hassan Firouzjahi, Moslem Zarei, Razieh Emami, S. M. Sadegh Movahed","submitted_at":"2010-10-26T19:29:35Z","abstract_excerpt":"We consider models of inflation with U(1) gauge fields and charged scalar fields including symmetry breaking potential, chaotic inflation and hybrid inflation. We show that there exist attractor solutions where the anisotropies produced during inflation becomes comparable to the slow-roll parameters. In the models where the inflaton field is a charged scalar field the gauge field becomes highly oscillatory at the end of inflation ending inflation quickly. Furthermore, in charged hybrid inflation the onset of waterfall phase transition at the end of inflation is affected significantly by the ev"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.5495","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":"2026-05-18T04:28:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iFpnEeE/fA12mDvTpWTwVcDDGLN9jK3lchV1e6HHJ7vkJBGHbAYKQUtJZKxg5CyQGNoPr/tx92iKvAJFERFEBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T11:51:12.963510Z"},"content_sha256":"c39ec604dd17dbe2d1981d26c78b08dda17697151ae3270466b8129f12d09b3b","schema_version":"1.0","event_id":"sha256:c39ec604dd17dbe2d1981d26c78b08dda17697151ae3270466b8129f12d09b3b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6CE6QSAZSSW3WQBVI4BCLP627G/bundle.json","state_url":"https://pith.science/pith/6CE6QSAZSSW3WQBVI4BCLP627G/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6CE6QSAZSSW3WQBVI4BCLP627G/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":"2026-08-01T11:51:12Z","links":{"resolver":"https://pith.science/pith/6CE6QSAZSSW3WQBVI4BCLP627G","bundle":"https://pith.science/pith/6CE6QSAZSSW3WQBVI4BCLP627G/bundle.json","state":"https://pith.science/pith/6CE6QSAZSSW3WQBVI4BCLP627G/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6CE6QSAZSSW3WQBVI4BCLP627G/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:6CE6QSAZSSW3WQBVI4BCLP627G","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":"6df72425b581d55909f89c6332d0ab44d041d000c35b43293973d262b309a2e5","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-10-26T19:29:35Z","title_canon_sha256":"3e41f6039c03ad7b2851459661f660de6151b72cb2d32cab296575b33bfa022a"},"schema_version":"1.0","source":{"id":"1010.5495","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.5495","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"arxiv_version","alias_value":"1010.5495v2","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.5495","created_at":"2026-05-18T04:28:29Z"},{"alias_kind":"pith_short_12","alias_value":"6CE6QSAZSSW3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6CE6QSAZSSW3WQBV","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6CE6QSAZ","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:c39ec604dd17dbe2d1981d26c78b08dda17697151ae3270466b8129f12d09b3b","target":"graph","created_at":"2026-05-18T04:28:29Z","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 consider models of inflation with U(1) gauge fields and charged scalar fields including symmetry breaking potential, chaotic inflation and hybrid inflation. We show that there exist attractor solutions where the anisotropies produced during inflation becomes comparable to the slow-roll parameters. In the models where the inflaton field is a charged scalar field the gauge field becomes highly oscillatory at the end of inflation ending inflation quickly. Furthermore, in charged hybrid inflation the onset of waterfall phase transition at the end of inflation is affected significantly by the ev","authors_text":"Hassan Firouzjahi, Moslem Zarei, Razieh Emami, S. M. Sadegh Movahed","cross_cats":["hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-10-26T19:29:35Z","title":"Anisotropic Inflation from Charged Scalar Fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.5495","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":"sha256:19fe37402a20e27dbdd6a1c6d44416eaaba75e9efa0b8dc031c2db5c7ef1b538","target":"record","created_at":"2026-05-18T04:28:29Z","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":"6df72425b581d55909f89c6332d0ab44d041d000c35b43293973d262b309a2e5","cross_cats_sorted":["hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2010-10-26T19:29:35Z","title_canon_sha256":"3e41f6039c03ad7b2851459661f660de6151b72cb2d32cab296575b33bfa022a"},"schema_version":"1.0","source":{"id":"1010.5495","kind":"arxiv","version":2}},"canonical_sha256":"f089e8481994adbb4035470225bfdaf998b29388930c612ea8c5e11f93b23a23","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f089e8481994adbb4035470225bfdaf998b29388930c612ea8c5e11f93b23a23","first_computed_at":"2026-05-18T04:28:29.337300Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:28:29.337300Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TcEGYEiBGSHgGKryMeCLnTaesmcPMKhiYGN9NYIeZa+5CKp6KG4oTqLonF8+fhs0NB0G4gLBlJCl3kx55O1RAA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:28:29.337660Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.5495","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:19fe37402a20e27dbdd6a1c6d44416eaaba75e9efa0b8dc031c2db5c7ef1b538","sha256:c39ec604dd17dbe2d1981d26c78b08dda17697151ae3270466b8129f12d09b3b"],"state_sha256":"2ea81893f3ce6a22dc885017fe7d0ba7de7af87943e8e4865febcbd7bf2d83ca"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cXr0z9C3sHVqzbwjB8XSbJ7jQG7O9vhoT6T1brLlzaXmc3AgRBpycf/6f/TpsuufIXTTclWprGhT2/DBg2PfCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-01T11:51:12.968660Z","bundle_sha256":"d26741cb12984e9506fe855e8cd704e64f314483da62fc7f703b68bf28c40804"}}