{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:TBRGN543JEYLUZQSPBTITEPZ73","short_pith_number":"pith:TBRGN543","canonical_record":{"source":{"id":"1708.03675","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-10T04:37:17Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6c570fa9c2e5a19b018fc5b3b92ecd951b36eeafeea91ec7e1276475b21724a2","abstract_canon_sha256":"3ff8248b909844a48cd9687421c7d66070341141f64aacad9e1c9ca3de5b6941"},"schema_version":"1.0"},"canonical_sha256":"986266f79b4930ba661278668991f9fed28f7b0695e358be14f94e8e8b3c339e","source":{"kind":"arxiv","id":"1708.03675","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.03675","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"arxiv_version","alias_value":"1708.03675v1","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.03675","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"pith_short_12","alias_value":"TBRGN543JEYL","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"TBRGN543JEYLUZQS","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"TBRGN543","created_at":"2026-05-18T12:31:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:TBRGN543JEYLUZQSPBTITEPZ73","target":"record","payload":{"canonical_record":{"source":{"id":"1708.03675","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-10T04:37:17Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6c570fa9c2e5a19b018fc5b3b92ecd951b36eeafeea91ec7e1276475b21724a2","abstract_canon_sha256":"3ff8248b909844a48cd9687421c7d66070341141f64aacad9e1c9ca3de5b6941"},"schema_version":"1.0"},"canonical_sha256":"986266f79b4930ba661278668991f9fed28f7b0695e358be14f94e8e8b3c339e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:08.172502Z","signature_b64":"UezeldtPOof4xE+WArw87MNj5QLb+4skEUVPBHmStV+U7GpSIfi/LAyweaUBBbyGfNaAQozeh+ILGyWYwLKWAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"986266f79b4930ba661278668991f9fed28f7b0695e358be14f94e8e8b3c339e","last_reissued_at":"2026-05-18T00:38:08.172110Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:08.172110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.03675","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":"2026-05-18T00:38:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kTN91ZHrjTuIZaH5H5nOLza5q7SVpbcSrcc+Z3wxCz4y8vEi7IexqVH6w0+5OcNGVZLJLlReOZjlsXqq18TvBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T01:51:17.006385Z"},"content_sha256":"aeaf824ee33c80158b303bd9ef1a0c0315fb21eb5d98cadf21c2245eda87d533","schema_version":"1.0","event_id":"sha256:aeaf824ee33c80158b303bd9ef1a0c0315fb21eb5d98cadf21c2245eda87d533"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:TBRGN543JEYLUZQSPBTITEPZ73","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Light of Planck-2015 on Non-Canonical Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"gr-qc","authors_text":"A. Mohammadi, Kh. Saaidi, T. Golanbari","submitted_at":"2017-08-10T04:37:17Z","abstract_excerpt":"Slow-roll inflationary scenario is considered in non-canonical scalar field model supposing a power-law function for kinetic term, and using two formalisms. In the first approach, the potential is considered as a power-law function, that is the most common approach in studying inflation. Hamilton-Jacobi approach is selected as the second formalism, so that the Hubble parameter is introduced as a function of scalar field instead of the potential. Employing the last observational data, the free parameters of the model are constrained, and the predicted form of the potential and attractor behavio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.03675","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":"2026-05-18T00:38:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PTOTpZ7i3dg7BVPwFu00lBjLEGULnRlyyNNt42KpDAfbutm5CwnDdawlANmVx5K96+TtcaHw9DUYsDXO7T73AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T01:51:17.007088Z"},"content_sha256":"c867aeee946b02738d9bd4d42c681b608702ca96daf191d39f2eef406f3f0b4c","schema_version":"1.0","event_id":"sha256:c867aeee946b02738d9bd4d42c681b608702ca96daf191d39f2eef406f3f0b4c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TBRGN543JEYLUZQSPBTITEPZ73/bundle.json","state_url":"https://pith.science/pith/TBRGN543JEYLUZQSPBTITEPZ73/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TBRGN543JEYLUZQSPBTITEPZ73/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":"2026-05-31T01:51:17Z","links":{"resolver":"https://pith.science/pith/TBRGN543JEYLUZQSPBTITEPZ73","bundle":"https://pith.science/pith/TBRGN543JEYLUZQSPBTITEPZ73/bundle.json","state":"https://pith.science/pith/TBRGN543JEYLUZQSPBTITEPZ73/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TBRGN543JEYLUZQSPBTITEPZ73/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:TBRGN543JEYLUZQSPBTITEPZ73","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":"3ff8248b909844a48cd9687421c7d66070341141f64aacad9e1c9ca3de5b6941","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-10T04:37:17Z","title_canon_sha256":"6c570fa9c2e5a19b018fc5b3b92ecd951b36eeafeea91ec7e1276475b21724a2"},"schema_version":"1.0","source":{"id":"1708.03675","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.03675","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"arxiv_version","alias_value":"1708.03675v1","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.03675","created_at":"2026-05-18T00:38:08Z"},{"alias_kind":"pith_short_12","alias_value":"TBRGN543JEYL","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"TBRGN543JEYLUZQS","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"TBRGN543","created_at":"2026-05-18T12:31:43Z"}],"graph_snapshots":[{"event_id":"sha256:c867aeee946b02738d9bd4d42c681b608702ca96daf191d39f2eef406f3f0b4c","target":"graph","created_at":"2026-05-18T00:38:08Z","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":"Slow-roll inflationary scenario is considered in non-canonical scalar field model supposing a power-law function for kinetic term, and using two formalisms. In the first approach, the potential is considered as a power-law function, that is the most common approach in studying inflation. Hamilton-Jacobi approach is selected as the second formalism, so that the Hubble parameter is introduced as a function of scalar field instead of the potential. Employing the last observational data, the free parameters of the model are constrained, and the predicted form of the potential and attractor behavio","authors_text":"A. Mohammadi, Kh. Saaidi, T. Golanbari","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-10T04:37:17Z","title":"Light of Planck-2015 on Non-Canonical Inflation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.03675","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:aeaf824ee33c80158b303bd9ef1a0c0315fb21eb5d98cadf21c2245eda87d533","target":"record","created_at":"2026-05-18T00:38:08Z","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":"3ff8248b909844a48cd9687421c7d66070341141f64aacad9e1c9ca3de5b6941","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-08-10T04:37:17Z","title_canon_sha256":"6c570fa9c2e5a19b018fc5b3b92ecd951b36eeafeea91ec7e1276475b21724a2"},"schema_version":"1.0","source":{"id":"1708.03675","kind":"arxiv","version":1}},"canonical_sha256":"986266f79b4930ba661278668991f9fed28f7b0695e358be14f94e8e8b3c339e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"986266f79b4930ba661278668991f9fed28f7b0695e358be14f94e8e8b3c339e","first_computed_at":"2026-05-18T00:38:08.172110Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:08.172110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UezeldtPOof4xE+WArw87MNj5QLb+4skEUVPBHmStV+U7GpSIfi/LAyweaUBBbyGfNaAQozeh+ILGyWYwLKWAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:08.172502Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.03675","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aeaf824ee33c80158b303bd9ef1a0c0315fb21eb5d98cadf21c2245eda87d533","sha256:c867aeee946b02738d9bd4d42c681b608702ca96daf191d39f2eef406f3f0b4c"],"state_sha256":"6f92d018cc4ea08905d95c27589679f1d5e4ee6b3652a282c26dd1261745864b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bu4QeNnQ0Hiuh4JQU5VL5HazTrn3EK5htwmNkoWECgXO28Twoaq6wdFxTFLzyS7wD30ojYmC8RACmM8lSqXFAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T01:51:17.010733Z","bundle_sha256":"538cdf02785fa8f7e93fb29f4acaeb46a98240b16129ce3bfee8bf73284c3765"}}