{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:BEE77E3FWPC7CLEV543W23ARCV","short_pith_number":"pith:BEE77E3F","canonical_record":{"source":{"id":"1504.07476","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T13:58:08Z","cross_cats_sorted":[],"title_canon_sha256":"e670c283c519a682c25ef254a6294dfc5e8890fd382873167da1d25ea91851a7","abstract_canon_sha256":"298f619fe615553f40f4d1e215604e39111407ecff92f428037b3f54bed7ef8d"},"schema_version":"1.0"},"canonical_sha256":"0909ff9365b3c5f12c95ef376d6c11156c03356370335ef9d4d75758d879a811","source":{"kind":"arxiv","id":"1504.07476","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.07476","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"arxiv_version","alias_value":"1504.07476v1","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.07476","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"pith_short_12","alias_value":"BEE77E3FWPC7","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"BEE77E3FWPC7CLEV","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"BEE77E3F","created_at":"2026-05-18T12:29:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:BEE77E3FWPC7CLEV543W23ARCV","target":"record","payload":{"canonical_record":{"source":{"id":"1504.07476","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T13:58:08Z","cross_cats_sorted":[],"title_canon_sha256":"e670c283c519a682c25ef254a6294dfc5e8890fd382873167da1d25ea91851a7","abstract_canon_sha256":"298f619fe615553f40f4d1e215604e39111407ecff92f428037b3f54bed7ef8d"},"schema_version":"1.0"},"canonical_sha256":"0909ff9365b3c5f12c95ef376d6c11156c03356370335ef9d4d75758d879a811","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:31.908658Z","signature_b64":"u+0Z9ntWh1OCkneVOeU+kH9YRDn/EGIu8h5GVV5QmWFHCE8tKPu/PSB81NbpTP/C6KpeXLLE+vGm+TC2Tcm2CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0909ff9365b3c5f12c95ef376d6c11156c03356370335ef9d4d75758d879a811","last_reissued_at":"2026-05-18T01:55:31.908018Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:31.908018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1504.07476","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:55:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PCMoIWLMf5u0E+/eizRcfL2VSEFG3px9s3PbxlANGljKM+dsMTsKOAWqYgliV4kXdsvex77jrprdswnzF+sGBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:32:00.762986Z"},"content_sha256":"087a592b54ba0b44362723b4c64f651925225059e489f45f45e14a937a250097","schema_version":"1.0","event_id":"sha256:087a592b54ba0b44362723b4c64f651925225059e489f45f45e14a937a250097"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:BEE77E3FWPC7CLEV543W23ARCV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Warm intermediate inflation in the Randall-Sundrum II model in the light of Planck 2015 and BICEP2 results: A general dissipative coefficient","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Marco Olivares, Nelson Videla, Ram\\'on Herrera","submitted_at":"2015-04-28T13:58:08Z","abstract_excerpt":"A warm inflationary Universe in the Randall-Sundrum II model during intermediate inflation is studied. For this purpose, we consider a general form for the dissipative coefficient $\\Gamma(T,\\phi)=C_{\\phi}\\,\\frac{T^{m}}{\\phi^{m-1}}$, and also analyze this inflationary model in the weak and strong dissipative regimes. We study the evolution of the Universe under the slow-roll approximation and find solutions to the full effective Friedmann equation in the brane-world framework. In order to constrain the parameters in our model, we consider the recent data from the BICEP2-Planck 2015 data togethe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.07476","kind":"arxiv","version":1},"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":"2026-05-18T01:55:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WHHuJFpuDB1D9tKz0P2+L3isIjjnTyjPxHn1Js5OFZkrR69/cGA4eVYOR5udInaBEphdRmNJQZHwIm4Qi2VwDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:32:00.763638Z"},"content_sha256":"ad74f9dd429c074ef4d402ba3937dff84cbd03bc0344ed411056d82d7be9baa5","schema_version":"1.0","event_id":"sha256:ad74f9dd429c074ef4d402ba3937dff84cbd03bc0344ed411056d82d7be9baa5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BEE77E3FWPC7CLEV543W23ARCV/bundle.json","state_url":"https://pith.science/pith/BEE77E3FWPC7CLEV543W23ARCV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BEE77E3FWPC7CLEV543W23ARCV/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":"2026-05-28T13:32:00Z","links":{"resolver":"https://pith.science/pith/BEE77E3FWPC7CLEV543W23ARCV","bundle":"https://pith.science/pith/BEE77E3FWPC7CLEV543W23ARCV/bundle.json","state":"https://pith.science/pith/BEE77E3FWPC7CLEV543W23ARCV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BEE77E3FWPC7CLEV543W23ARCV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:BEE77E3FWPC7CLEV543W23ARCV","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":"298f619fe615553f40f4d1e215604e39111407ecff92f428037b3f54bed7ef8d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T13:58:08Z","title_canon_sha256":"e670c283c519a682c25ef254a6294dfc5e8890fd382873167da1d25ea91851a7"},"schema_version":"1.0","source":{"id":"1504.07476","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.07476","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"arxiv_version","alias_value":"1504.07476v1","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.07476","created_at":"2026-05-18T01:55:31Z"},{"alias_kind":"pith_short_12","alias_value":"BEE77E3FWPC7","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"BEE77E3FWPC7CLEV","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"BEE77E3F","created_at":"2026-05-18T12:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:ad74f9dd429c074ef4d402ba3937dff84cbd03bc0344ed411056d82d7be9baa5","target":"graph","created_at":"2026-05-18T01:55:31Z","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":"A warm inflationary Universe in the Randall-Sundrum II model during intermediate inflation is studied. For this purpose, we consider a general form for the dissipative coefficient $\\Gamma(T,\\phi)=C_{\\phi}\\,\\frac{T^{m}}{\\phi^{m-1}}$, and also analyze this inflationary model in the weak and strong dissipative regimes. We study the evolution of the Universe under the slow-roll approximation and find solutions to the full effective Friedmann equation in the brane-world framework. In order to constrain the parameters in our model, we consider the recent data from the BICEP2-Planck 2015 data togethe","authors_text":"Marco Olivares, Nelson Videla, Ram\\'on Herrera","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T13:58:08Z","title":"Warm intermediate inflation in the Randall-Sundrum II model in the light of Planck 2015 and BICEP2 results: A general dissipative coefficient"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.07476","kind":"arxiv","version":1},"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":"sha256:087a592b54ba0b44362723b4c64f651925225059e489f45f45e14a937a250097","target":"record","created_at":"2026-05-18T01:55:31Z","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":"298f619fe615553f40f4d1e215604e39111407ecff92f428037b3f54bed7ef8d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-28T13:58:08Z","title_canon_sha256":"e670c283c519a682c25ef254a6294dfc5e8890fd382873167da1d25ea91851a7"},"schema_version":"1.0","source":{"id":"1504.07476","kind":"arxiv","version":1}},"canonical_sha256":"0909ff9365b3c5f12c95ef376d6c11156c03356370335ef9d4d75758d879a811","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0909ff9365b3c5f12c95ef376d6c11156c03356370335ef9d4d75758d879a811","first_computed_at":"2026-05-18T01:55:31.908018Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:55:31.908018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u+0Z9ntWh1OCkneVOeU+kH9YRDn/EGIu8h5GVV5QmWFHCE8tKPu/PSB81NbpTP/C6KpeXLLE+vGm+TC2Tcm2CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:55:31.908658Z","signed_message":"canonical_sha256_bytes"},"source_id":"1504.07476","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:087a592b54ba0b44362723b4c64f651925225059e489f45f45e14a937a250097","sha256:ad74f9dd429c074ef4d402ba3937dff84cbd03bc0344ed411056d82d7be9baa5"],"state_sha256":"713615f7c88b025ba30fac8a30fd1210f269f01760006230902f3f904738fd05"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7qKTHTwwFPtCixESC79kww/68d3djX7j+y8sSyIt2KAgNBFiqYsvaHDTrXrJKeE1NmAiKvgEW4dRhBg99g6nCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T13:32:00.766714Z","bundle_sha256":"2a04f3407db94d189c9747e2db401cc44b00d4c41c999333a3f59c894b79eca1"}}