{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:C2ZJL4PVO3I3FV573LU24QE2PQ","short_pith_number":"pith:C2ZJL4PV","canonical_record":{"source":{"id":"1505.04390","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-17T12:28:34Z","cross_cats_sorted":[],"title_canon_sha256":"cb818383aaf8daab098bb383ed7ae852834db370d9e275636e34a0a31b1621dd","abstract_canon_sha256":"8ea2f4188d8a825a8e43065a3d3f47df8a28219cebf06f98c9a14abcfa8c5701"},"schema_version":"1.0"},"canonical_sha256":"16b295f1f576d1b2d7bfdae9ae409a7c0f7d2b9e9f2148b0284d3c17df8b04f9","source":{"kind":"arxiv","id":"1505.04390","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.04390","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"arxiv_version","alias_value":"1505.04390v3","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.04390","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"pith_short_12","alias_value":"C2ZJL4PVO3I3","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"C2ZJL4PVO3I3FV57","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"C2ZJL4PV","created_at":"2026-05-18T12:29:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:C2ZJL4PVO3I3FV573LU24QE2PQ","target":"record","payload":{"canonical_record":{"source":{"id":"1505.04390","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-17T12:28:34Z","cross_cats_sorted":[],"title_canon_sha256":"cb818383aaf8daab098bb383ed7ae852834db370d9e275636e34a0a31b1621dd","abstract_canon_sha256":"8ea2f4188d8a825a8e43065a3d3f47df8a28219cebf06f98c9a14abcfa8c5701"},"schema_version":"1.0"},"canonical_sha256":"16b295f1f576d1b2d7bfdae9ae409a7c0f7d2b9e9f2148b0284d3c17df8b04f9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:25.710758Z","signature_b64":"1RY5btLoWBKpraMV0Zz9GljUok9Q0tZXqDEXkCGNUSd1p2H8gkc6AixKKkC3aM4E5dWcDWUqtQ9gxkfK4ZPgBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"16b295f1f576d1b2d7bfdae9ae409a7c0f7d2b9e9f2148b0284d3c17df8b04f9","last_reissued_at":"2026-05-18T01:17:25.710259Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:25.710259Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.04390","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":"2026-05-18T01:17:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cPkn7/6j6Qj7lLdwB6AMt7CbuUl1nbY2CurkBBKNbM4IHMp12F6a6b4i0WXpoZsW2RuF760yZ4rSmg8b/hGRBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T12:04:11.373110Z"},"content_sha256":"3912c417e0dc0b85584c19f4378641e16feceeadedf6897bd719ebb1e10e47a7","schema_version":"1.0","event_id":"sha256:3912c417e0dc0b85584c19f4378641e16feceeadedf6897bd719ebb1e10e47a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:C2ZJL4PVO3I3FV573LU24QE2PQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-minimal kinetic coupled gravity: inflation on the Warped DGP brane","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"A. Parsiya, F. Darabi, K. Atazadeh","submitted_at":"2015-05-17T12:28:34Z","abstract_excerpt":"We consider the non-minimally kinetic coupled version of DGP brane model, where the kinetic term of the scalar field is coupled to the metric and Einstein tensor on the brane by a coupling constant $\\zeta$. We obtain the corresponding field equations, using the Friedmann-Robertson-Walker metric and the perfect fluid, and study the inflationary scenario to confront the numerical analysis of six typical scalar field potentials with the current observational results. We find that among the suggested potentials and coupling constants, subject to the e-folding $N=60$, the potentials $V(\\phi)=\\sigma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.04390","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":"2026-05-18T01:17:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"85PdC6gaSsVqD6TvQ8ooHwoXrWOjrAVK/QY9dofHAVmjk2wJs3PsMkf0IaLh0b4+HxjrTh8ERbZ9TDmA+Pm6BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T12:04:11.373767Z"},"content_sha256":"366453f51361ade58f7b9b4dcd0be209182a262933bf4cadb70b95dc9d47b697","schema_version":"1.0","event_id":"sha256:366453f51361ade58f7b9b4dcd0be209182a262933bf4cadb70b95dc9d47b697"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/bundle.json","state_url":"https://pith.science/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/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":"2026-05-30T12:04:11Z","links":{"resolver":"https://pith.science/pith/C2ZJL4PVO3I3FV573LU24QE2PQ","bundle":"https://pith.science/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/bundle.json","state":"https://pith.science/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C2ZJL4PVO3I3FV573LU24QE2PQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:C2ZJL4PVO3I3FV573LU24QE2PQ","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":"8ea2f4188d8a825a8e43065a3d3f47df8a28219cebf06f98c9a14abcfa8c5701","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-17T12:28:34Z","title_canon_sha256":"cb818383aaf8daab098bb383ed7ae852834db370d9e275636e34a0a31b1621dd"},"schema_version":"1.0","source":{"id":"1505.04390","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.04390","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"arxiv_version","alias_value":"1505.04390v3","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.04390","created_at":"2026-05-18T01:17:25Z"},{"alias_kind":"pith_short_12","alias_value":"C2ZJL4PVO3I3","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"C2ZJL4PVO3I3FV57","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"C2ZJL4PV","created_at":"2026-05-18T12:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:366453f51361ade58f7b9b4dcd0be209182a262933bf4cadb70b95dc9d47b697","target":"graph","created_at":"2026-05-18T01:17:25Z","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 the non-minimally kinetic coupled version of DGP brane model, where the kinetic term of the scalar field is coupled to the metric and Einstein tensor on the brane by a coupling constant $\\zeta$. We obtain the corresponding field equations, using the Friedmann-Robertson-Walker metric and the perfect fluid, and study the inflationary scenario to confront the numerical analysis of six typical scalar field potentials with the current observational results. We find that among the suggested potentials and coupling constants, subject to the e-folding $N=60$, the potentials $V(\\phi)=\\sigma","authors_text":"A. Parsiya, F. Darabi, K. Atazadeh","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-17T12:28:34Z","title":"Non-minimal kinetic coupled gravity: inflation on the Warped DGP brane"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.04390","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":"sha256:3912c417e0dc0b85584c19f4378641e16feceeadedf6897bd719ebb1e10e47a7","target":"record","created_at":"2026-05-18T01:17:25Z","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":"8ea2f4188d8a825a8e43065a3d3f47df8a28219cebf06f98c9a14abcfa8c5701","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-17T12:28:34Z","title_canon_sha256":"cb818383aaf8daab098bb383ed7ae852834db370d9e275636e34a0a31b1621dd"},"schema_version":"1.0","source":{"id":"1505.04390","kind":"arxiv","version":3}},"canonical_sha256":"16b295f1f576d1b2d7bfdae9ae409a7c0f7d2b9e9f2148b0284d3c17df8b04f9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"16b295f1f576d1b2d7bfdae9ae409a7c0f7d2b9e9f2148b0284d3c17df8b04f9","first_computed_at":"2026-05-18T01:17:25.710259Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:25.710259Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1RY5btLoWBKpraMV0Zz9GljUok9Q0tZXqDEXkCGNUSd1p2H8gkc6AixKKkC3aM4E5dWcDWUqtQ9gxkfK4ZPgBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:25.710758Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.04390","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3912c417e0dc0b85584c19f4378641e16feceeadedf6897bd719ebb1e10e47a7","sha256:366453f51361ade58f7b9b4dcd0be209182a262933bf4cadb70b95dc9d47b697"],"state_sha256":"e67d16c9454cb8fced6370d1d0ca1131e43541bebf37dd4c6a485cace8afc574"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k1uLSU0FuXcmzskDVzfYlmhqmcZ9E3XDdKbGuv/wcfVhfL6EkHwRlNC1v0LU/jtznvvc/RKMBYSTWMa+DGXRCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T12:04:11.376692Z","bundle_sha256":"c899e4eedfb586e80dbfa9a11f23af80f0b9b7b7c875c0eb639fc57165aa0c3f"}}