{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:32TGOEI67I5CKLQGTOUVJP6HXV","short_pith_number":"pith:32TGOEI6","canonical_record":{"source":{"id":"1710.00682","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-28T09:16:24Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"63ef90a956700677945cd93aef2e9a79a7e6286c2ade3fe703660d9ec68dfba8","abstract_canon_sha256":"d31508db86a58401b35799a785e9b8525b2eaaca4e377fcd649332da4cefbc77"},"schema_version":"1.0"},"canonical_sha256":"dea667111efa3a252e069ba954bfc7bd7f527ca8eb2f8d5fb8e06b8b64f61ce5","source":{"kind":"arxiv","id":"1710.00682","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.00682","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"arxiv_version","alias_value":"1710.00682v3","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.00682","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"pith_short_12","alias_value":"32TGOEI67I5C","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"32TGOEI67I5CKLQG","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"32TGOEI6","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:32TGOEI67I5CKLQGTOUVJP6HXV","target":"record","payload":{"canonical_record":{"source":{"id":"1710.00682","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-28T09:16:24Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"63ef90a956700677945cd93aef2e9a79a7e6286c2ade3fe703660d9ec68dfba8","abstract_canon_sha256":"d31508db86a58401b35799a785e9b8525b2eaaca4e377fcd649332da4cefbc77"},"schema_version":"1.0"},"canonical_sha256":"dea667111efa3a252e069ba954bfc7bd7f527ca8eb2f8d5fb8e06b8b64f61ce5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:47.417878Z","signature_b64":"ZaVoKNf24t+esMGMSZsyCewyV6UI39AU481I0CSdYchPZtohlvMNPbOIZjAWIsZeYv+/NyjHJL6D9AKmwMJpBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dea667111efa3a252e069ba954bfc7bd7f527ca8eb2f8d5fb8e06b8b64f61ce5","last_reissued_at":"2026-05-18T00:10:47.417189Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:47.417189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.00682","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":"2026-05-18T00:10:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d1a4uF19PKQhay91OWbU25tltBXxAByGZ2FDNr9/X4lDQa64vWBL1Sc9ruTzIKGMbONZ+JAlBjYaDd8Kkc7gBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T13:58:47.921643Z"},"content_sha256":"9caa3f1d3719b7fe491533801b86735020fa2364694662c13acd585501ac5585","schema_version":"1.0","event_id":"sha256:9caa3f1d3719b7fe491533801b86735020fa2364694662c13acd585501ac5585"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:32TGOEI67I5CKLQGTOUVJP6HXV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Constant-roll Inflation in $f(T)$ Teleparallel Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"A. Awad, G.G.L. Nashed, S.D. Odintsov, V.K. Oikonomou, W. El Hanafy","submitted_at":"2017-09-28T09:16:24Z","abstract_excerpt":"We investigate in detail the implications of the constant-roll condition on the inflationary era of a scalar field coupled to a teleparallel $f(T)$ gravity. The resulting cosmological equations constitute a reconstruction technique which enables us to find either the $f(T)$ gravity which corresponds to a given cosmological evolution, or the Hubble rate of the cosmological evolution generated by a fixed $f(T)$ gravity. We also analyze in some detail the phase space of the constant-roll teleparallel gravity and we discuss the physical significance of the resulting fixed points and trajectories. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.00682","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":"2026-05-18T00:10:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wzDlmOCk08RLxTELDCwnat2k+jcck7uMfGuNjLrgBtSTRpny3AgyRnZooKoIgTr2IPnSrLnZ8JFqnj208JOzCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T13:58:47.921991Z"},"content_sha256":"d335128edd2daa8b850805d77aa80dfd63473b30936953e17c97508ca3082ec3","schema_version":"1.0","event_id":"sha256:d335128edd2daa8b850805d77aa80dfd63473b30936953e17c97508ca3082ec3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/32TGOEI67I5CKLQGTOUVJP6HXV/bundle.json","state_url":"https://pith.science/pith/32TGOEI67I5CKLQGTOUVJP6HXV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/32TGOEI67I5CKLQGTOUVJP6HXV/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":"2026-06-05T13:58:47Z","links":{"resolver":"https://pith.science/pith/32TGOEI67I5CKLQGTOUVJP6HXV","bundle":"https://pith.science/pith/32TGOEI67I5CKLQGTOUVJP6HXV/bundle.json","state":"https://pith.science/pith/32TGOEI67I5CKLQGTOUVJP6HXV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/32TGOEI67I5CKLQGTOUVJP6HXV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:32TGOEI67I5CKLQGTOUVJP6HXV","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":"d31508db86a58401b35799a785e9b8525b2eaaca4e377fcd649332da4cefbc77","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-28T09:16:24Z","title_canon_sha256":"63ef90a956700677945cd93aef2e9a79a7e6286c2ade3fe703660d9ec68dfba8"},"schema_version":"1.0","source":{"id":"1710.00682","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.00682","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"arxiv_version","alias_value":"1710.00682v3","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.00682","created_at":"2026-05-18T00:10:47Z"},{"alias_kind":"pith_short_12","alias_value":"32TGOEI67I5C","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"32TGOEI67I5CKLQG","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"32TGOEI6","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:d335128edd2daa8b850805d77aa80dfd63473b30936953e17c97508ca3082ec3","target":"graph","created_at":"2026-05-18T00:10:47Z","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 investigate in detail the implications of the constant-roll condition on the inflationary era of a scalar field coupled to a teleparallel $f(T)$ gravity. The resulting cosmological equations constitute a reconstruction technique which enables us to find either the $f(T)$ gravity which corresponds to a given cosmological evolution, or the Hubble rate of the cosmological evolution generated by a fixed $f(T)$ gravity. We also analyze in some detail the phase space of the constant-roll teleparallel gravity and we discuss the physical significance of the resulting fixed points and trajectories. ","authors_text":"A. Awad, G.G.L. Nashed, S.D. Odintsov, V.K. Oikonomou, W. El Hanafy","cross_cats":["astro-ph.CO","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-28T09:16:24Z","title":"Constant-roll Inflation in $f(T)$ Teleparallel Gravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.00682","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":"sha256:9caa3f1d3719b7fe491533801b86735020fa2364694662c13acd585501ac5585","target":"record","created_at":"2026-05-18T00:10:47Z","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":"d31508db86a58401b35799a785e9b8525b2eaaca4e377fcd649332da4cefbc77","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-28T09:16:24Z","title_canon_sha256":"63ef90a956700677945cd93aef2e9a79a7e6286c2ade3fe703660d9ec68dfba8"},"schema_version":"1.0","source":{"id":"1710.00682","kind":"arxiv","version":3}},"canonical_sha256":"dea667111efa3a252e069ba954bfc7bd7f527ca8eb2f8d5fb8e06b8b64f61ce5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dea667111efa3a252e069ba954bfc7bd7f527ca8eb2f8d5fb8e06b8b64f61ce5","first_computed_at":"2026-05-18T00:10:47.417189Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:10:47.417189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZaVoKNf24t+esMGMSZsyCewyV6UI39AU481I0CSdYchPZtohlvMNPbOIZjAWIsZeYv+/NyjHJL6D9AKmwMJpBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:10:47.417878Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.00682","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9caa3f1d3719b7fe491533801b86735020fa2364694662c13acd585501ac5585","sha256:d335128edd2daa8b850805d77aa80dfd63473b30936953e17c97508ca3082ec3"],"state_sha256":"a6afea47943b0711864219172ac995341dd3fe4fd8961c792e6d711b477900f0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r2QUCzw7G0UQNst8yvWU4b1Nby3xUexr21e7Y4gBNgq2nXKqGdnOj614fD/E47CQeq4cZf/3VS6AiNxqU1UjAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T13:58:47.924002Z","bundle_sha256":"72dd2bbbf9784648319f52790b0e6230dae9a2b16e4a09bbabe78f338160031b"}}