{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:GO3DMWGN6AXLHUPA4JQS45LIHI","short_pith_number":"pith:GO3DMWGN","canonical_record":{"source":{"id":"1302.1103","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-02-05T16:36:47Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ce0e4535da47a61bbe18601ba8d40db1804b6153611c480c5fab2cdd141378cb","abstract_canon_sha256":"c99757d9ab2db3874ba1838946a86b1fbb0c49b2ce9903b5ecfe4d155490f7c6"},"schema_version":"1.0"},"canonical_sha256":"33b63658cdf02eb3d1e0e2612e75683a1c0563f99a6fb7e7b455f305efd6d414","source":{"kind":"arxiv","id":"1302.1103","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.1103","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"arxiv_version","alias_value":"1302.1103v2","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.1103","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"pith_short_12","alias_value":"GO3DMWGN6AXL","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GO3DMWGN6AXLHUPA","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GO3DMWGN","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:GO3DMWGN6AXLHUPA4JQS45LIHI","target":"record","payload":{"canonical_record":{"source":{"id":"1302.1103","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-02-05T16:36:47Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ce0e4535da47a61bbe18601ba8d40db1804b6153611c480c5fab2cdd141378cb","abstract_canon_sha256":"c99757d9ab2db3874ba1838946a86b1fbb0c49b2ce9903b5ecfe4d155490f7c6"},"schema_version":"1.0"},"canonical_sha256":"33b63658cdf02eb3d1e0e2612e75683a1c0563f99a6fb7e7b455f305efd6d414","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:51:50.226993Z","signature_b64":"TaEn3Qhv7WkdFo/y3mQcuOavSaw5Z48csCH0FxUpVHW5qzC+HWnjkcv5TEcP3h4V+uniecgbdCHvKEQAvGjuCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33b63658cdf02eb3d1e0e2612e75683a1c0563f99a6fb7e7b455f305efd6d414","last_reissued_at":"2026-05-18T01:51:50.226583Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:51:50.226583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.1103","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:51:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8CBXdoJz0mET4nNyku+5GKuS89Zu761pPv3broqf35CvfOLBQDJQHtV4Y9oWsp09z4WovoYOvPvBJDR0M/jYBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T09:15:39.570207Z"},"content_sha256":"fadce4fc042d4ddae2d9126c83f4d55d3032d08f37e702242e3d58293bff7f3b","schema_version":"1.0","event_id":"sha256:fadce4fc042d4ddae2d9126c83f4d55d3032d08f37e702242e3d58293bff7f3b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:GO3DMWGN6AXLHUPA4JQS45LIHI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exploring Cartan gravity with dynamical symmetry breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"H.F. Westman, T.G. Zlosnik","submitted_at":"2013-02-05T16:36:47Z","abstract_excerpt":"It has been known for some time that General Relativity can be regarded as a Yang-Mills-type gauge theory in a symmetry broken phase. In this picture the gravity sector is described by an $SO(1,4)$ or $SO(2,3)$ gauge field $A^{a}_{\\phantom{a}b\\mu}$ and Higgs field $V^{a}$ which acts to break the symmetry down to that of the Lorentz group $SO(1,3)$. This symmetry breaking mirrors that of electroweak theory. However, a notable difference is that while the Higgs field $\\Phi$ of electroweak theory is taken as a genuine dynamical field satisfying a Klein-Gordon equation, the gauge independent norm "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.1103","kind":"arxiv","version":2},"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":"2026-05-18T01:51:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YCCGulg2CX4Qfq3/DLQHU/qEGEZX86G+HZCXrrD434k5+g3i3YorZnBQhsdugS//fzMym34V6MFXNShzgh7kDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T09:15:39.570669Z"},"content_sha256":"21eecb420c00c2673057522341794fe3e8c841640bc8f86170622c690e92418a","schema_version":"1.0","event_id":"sha256:21eecb420c00c2673057522341794fe3e8c841640bc8f86170622c690e92418a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/bundle.json","state_url":"https://pith.science/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/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":"2026-08-19T09:15:39Z","links":{"resolver":"https://pith.science/pith/GO3DMWGN6AXLHUPA4JQS45LIHI","bundle":"https://pith.science/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/bundle.json","state":"https://pith.science/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GO3DMWGN6AXLHUPA4JQS45LIHI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:GO3DMWGN6AXLHUPA4JQS45LIHI","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":"c99757d9ab2db3874ba1838946a86b1fbb0c49b2ce9903b5ecfe4d155490f7c6","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-02-05T16:36:47Z","title_canon_sha256":"ce0e4535da47a61bbe18601ba8d40db1804b6153611c480c5fab2cdd141378cb"},"schema_version":"1.0","source":{"id":"1302.1103","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.1103","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"arxiv_version","alias_value":"1302.1103v2","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.1103","created_at":"2026-05-18T01:51:50Z"},{"alias_kind":"pith_short_12","alias_value":"GO3DMWGN6AXL","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GO3DMWGN6AXLHUPA","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GO3DMWGN","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:21eecb420c00c2673057522341794fe3e8c841640bc8f86170622c690e92418a","target":"graph","created_at":"2026-05-18T01:51:50Z","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":"It has been known for some time that General Relativity can be regarded as a Yang-Mills-type gauge theory in a symmetry broken phase. In this picture the gravity sector is described by an $SO(1,4)$ or $SO(2,3)$ gauge field $A^{a}_{\\phantom{a}b\\mu}$ and Higgs field $V^{a}$ which acts to break the symmetry down to that of the Lorentz group $SO(1,3)$. This symmetry breaking mirrors that of electroweak theory. However, a notable difference is that while the Higgs field $\\Phi$ of electroweak theory is taken as a genuine dynamical field satisfying a Klein-Gordon equation, the gauge independent norm ","authors_text":"H.F. Westman, T.G. Zlosnik","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-02-05T16:36:47Z","title":"Exploring Cartan gravity with dynamical symmetry breaking"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.1103","kind":"arxiv","version":2},"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:fadce4fc042d4ddae2d9126c83f4d55d3032d08f37e702242e3d58293bff7f3b","target":"record","created_at":"2026-05-18T01:51:50Z","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":"c99757d9ab2db3874ba1838946a86b1fbb0c49b2ce9903b5ecfe4d155490f7c6","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-02-05T16:36:47Z","title_canon_sha256":"ce0e4535da47a61bbe18601ba8d40db1804b6153611c480c5fab2cdd141378cb"},"schema_version":"1.0","source":{"id":"1302.1103","kind":"arxiv","version":2}},"canonical_sha256":"33b63658cdf02eb3d1e0e2612e75683a1c0563f99a6fb7e7b455f305efd6d414","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"33b63658cdf02eb3d1e0e2612e75683a1c0563f99a6fb7e7b455f305efd6d414","first_computed_at":"2026-05-18T01:51:50.226583Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:51:50.226583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TaEn3Qhv7WkdFo/y3mQcuOavSaw5Z48csCH0FxUpVHW5qzC+HWnjkcv5TEcP3h4V+uniecgbdCHvKEQAvGjuCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:51:50.226993Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.1103","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fadce4fc042d4ddae2d9126c83f4d55d3032d08f37e702242e3d58293bff7f3b","sha256:21eecb420c00c2673057522341794fe3e8c841640bc8f86170622c690e92418a"],"state_sha256":"561d5f4be4e6864a1455244cccf89d4b57f4a3fa3c4ca0026b9ccde9ab62ef28"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"szNMjEBJ4Fy9nR1QCU5fTo0gcxyPcevU2aqSkSZTkrYsRlnKSj0nLOuiOZ/fTZLkCykuEyJb25UrYtjzMBECBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-19T09:15:39.588359Z","bundle_sha256":"e70732e43d346c6917517e166e9a76bcccb4db4d259ea02e228c28b8fab47e8d"}}