{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:Z7NDK63HK4I6CX5QULW7QM4HSB","short_pith_number":"pith:Z7NDK63H","canonical_record":{"source":{"id":"1606.06963","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-05-17T09:31:45Z","cross_cats_sorted":[],"title_canon_sha256":"652b1a7de0695e9a9fae2ff70646d211489a3cf115d574436f5f95f6540b3d42","abstract_canon_sha256":"cd04e2723df84c57cce7246174b90135e397d774209d6aaa19ff1ff335a8bcf7"},"schema_version":"1.0"},"canonical_sha256":"cfda357b675711e15fb0a2edf833879051f99c4fad0f74121c9bfa0f7a7bf2bc","source":{"kind":"arxiv","id":"1606.06963","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.06963","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"arxiv_version","alias_value":"1606.06963v3","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.06963","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"pith_short_12","alias_value":"Z7NDK63HK4I6","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"Z7NDK63HK4I6CX5Q","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"Z7NDK63H","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:Z7NDK63HK4I6CX5QULW7QM4HSB","target":"record","payload":{"canonical_record":{"source":{"id":"1606.06963","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-05-17T09:31:45Z","cross_cats_sorted":[],"title_canon_sha256":"652b1a7de0695e9a9fae2ff70646d211489a3cf115d574436f5f95f6540b3d42","abstract_canon_sha256":"cd04e2723df84c57cce7246174b90135e397d774209d6aaa19ff1ff335a8bcf7"},"schema_version":"1.0"},"canonical_sha256":"cfda357b675711e15fb0a2edf833879051f99c4fad0f74121c9bfa0f7a7bf2bc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:40.506879Z","signature_b64":"xQTj7CeueD82Kh8SuQeNxxbSfr7ik4PZ0Hebc7QK7SAm/AYfg9e0EnVotE9n/gQbKStOaoN0GHg8i2FbvJiCCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cfda357b675711e15fb0a2edf833879051f99c4fad0f74121c9bfa0f7a7bf2bc","last_reissued_at":"2026-05-18T01:06:40.506126Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:40.506126Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.06963","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":"2026-05-18T01:06:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JFkUNmoZVrCNut7I4UvqJfbn2Q910uYlJd9piJgnXTYWxAw8L0vQOdPW0bWFtkrvQ07UErR3lekdJ1teoh14BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T12:35:38.679138Z"},"content_sha256":"d981a55e42e919a0ded6b592c46c6de5bf42c61bf3dcb8d79c5190bf756c036d","schema_version":"1.0","event_id":"sha256:d981a55e42e919a0ded6b592c46c6de5bf42c61bf3dcb8d79c5190bf756c036d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:Z7NDK63HK4I6CX5QULW7QM4HSB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strong Gravity Approach to QCD and General Relativity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Farida Tahir, O. F. Akinto","submitted_at":"2016-05-17T09:31:45Z","abstract_excerpt":"A systematic study of the Weyl-type / Yang-Mills-type action possessing local conformal invariance and quadratic curvature is undertaken. The dynamical breaking of this conformal invariance / scale invariance induces general relativity (GR) as an effective long distance limit of the theory. We prove that the corresponding field equations of the theory have the linearly rising potential, which naturally possesses asymptotic freedom and color confinement properties of quantum chromodynamics (QCD). Solutions to the neutrino mass and dark energy problems come as free gifts of this formulation. Thi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.06963","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":"2026-05-18T01:06:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JJX/Z38Bt2xknNFDyLzO0/MrWH7sJ107aZmA9KObDt6dDvkKrGcIzLnzMzzXbBHnKosxAm43UN2CA+6DIddWBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T12:35:38.679542Z"},"content_sha256":"ae00d54af8e3fb60cd9eb2290225e24dccf18f98bdae5c407ab66a0d1a1111f8","schema_version":"1.0","event_id":"sha256:ae00d54af8e3fb60cd9eb2290225e24dccf18f98bdae5c407ab66a0d1a1111f8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/bundle.json","state_url":"https://pith.science/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/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":"2026-07-03T12:35:38Z","links":{"resolver":"https://pith.science/pith/Z7NDK63HK4I6CX5QULW7QM4HSB","bundle":"https://pith.science/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/bundle.json","state":"https://pith.science/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Z7NDK63HK4I6CX5QULW7QM4HSB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:Z7NDK63HK4I6CX5QULW7QM4HSB","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":"cd04e2723df84c57cce7246174b90135e397d774209d6aaa19ff1ff335a8bcf7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-05-17T09:31:45Z","title_canon_sha256":"652b1a7de0695e9a9fae2ff70646d211489a3cf115d574436f5f95f6540b3d42"},"schema_version":"1.0","source":{"id":"1606.06963","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.06963","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"arxiv_version","alias_value":"1606.06963v3","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.06963","created_at":"2026-05-18T01:06:40Z"},{"alias_kind":"pith_short_12","alias_value":"Z7NDK63HK4I6","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"Z7NDK63HK4I6CX5Q","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"Z7NDK63H","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:ae00d54af8e3fb60cd9eb2290225e24dccf18f98bdae5c407ab66a0d1a1111f8","target":"graph","created_at":"2026-05-18T01:06:40Z","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 systematic study of the Weyl-type / Yang-Mills-type action possessing local conformal invariance and quadratic curvature is undertaken. The dynamical breaking of this conformal invariance / scale invariance induces general relativity (GR) as an effective long distance limit of the theory. We prove that the corresponding field equations of the theory have the linearly rising potential, which naturally possesses asymptotic freedom and color confinement properties of quantum chromodynamics (QCD). Solutions to the neutrino mass and dark energy problems come as free gifts of this formulation. Thi","authors_text":"Farida Tahir, O. F. Akinto","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-05-17T09:31:45Z","title":"Strong Gravity Approach to QCD and General Relativity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.06963","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:d981a55e42e919a0ded6b592c46c6de5bf42c61bf3dcb8d79c5190bf756c036d","target":"record","created_at":"2026-05-18T01:06:40Z","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":"cd04e2723df84c57cce7246174b90135e397d774209d6aaa19ff1ff335a8bcf7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2016-05-17T09:31:45Z","title_canon_sha256":"652b1a7de0695e9a9fae2ff70646d211489a3cf115d574436f5f95f6540b3d42"},"schema_version":"1.0","source":{"id":"1606.06963","kind":"arxiv","version":3}},"canonical_sha256":"cfda357b675711e15fb0a2edf833879051f99c4fad0f74121c9bfa0f7a7bf2bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cfda357b675711e15fb0a2edf833879051f99c4fad0f74121c9bfa0f7a7bf2bc","first_computed_at":"2026-05-18T01:06:40.506126Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:40.506126Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xQTj7CeueD82Kh8SuQeNxxbSfr7ik4PZ0Hebc7QK7SAm/AYfg9e0EnVotE9n/gQbKStOaoN0GHg8i2FbvJiCCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:40.506879Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.06963","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d981a55e42e919a0ded6b592c46c6de5bf42c61bf3dcb8d79c5190bf756c036d","sha256:ae00d54af8e3fb60cd9eb2290225e24dccf18f98bdae5c407ab66a0d1a1111f8"],"state_sha256":"571a20da3039ba25d64f39777c9c6bd56b11628ec894c1494ab6ccd7929aa44c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nYl4JuZw08+uc9wkBL1lmGBuFnG6A63m0Y2En8Z/Hc5NDeeC6B1kf9tv3mNwfPoHOQ1isbIGQCvhIcda9XUbCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-03T12:35:38.681451Z","bundle_sha256":"9ab3020828d0b895509080a10880efdd425079ca62214a4a06d73adebe0e59f2"}}