{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:2YWDZIZ7MPMBEHIQVZCQSFLAQ2","short_pith_number":"pith:2YWDZIZ7","canonical_record":{"source":{"id":"1104.2830","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-14T16:54:55Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"431bd525ae8ccc2ce1322f1be1fc878c177836d28aa37fd8f1a072f9e657ae89","abstract_canon_sha256":"890ed3092ebd7b32c96d1f879032e89a04b92addb12906bc4bce88b78c9fc22a"},"schema_version":"1.0"},"canonical_sha256":"d62c3ca33f63d8121d10ae4509156086a8c034f707080842760488fe59d37a30","source":{"kind":"arxiv","id":"1104.2830","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.2830","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"arxiv_version","alias_value":"1104.2830v2","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.2830","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"pith_short_12","alias_value":"2YWDZIZ7MPMB","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"2YWDZIZ7MPMBEHIQ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"2YWDZIZ7","created_at":"2026-05-18T12:26:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:2YWDZIZ7MPMBEHIQVZCQSFLAQ2","target":"record","payload":{"canonical_record":{"source":{"id":"1104.2830","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-14T16:54:55Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"431bd525ae8ccc2ce1322f1be1fc878c177836d28aa37fd8f1a072f9e657ae89","abstract_canon_sha256":"890ed3092ebd7b32c96d1f879032e89a04b92addb12906bc4bce88b78c9fc22a"},"schema_version":"1.0"},"canonical_sha256":"d62c3ca33f63d8121d10ae4509156086a8c034f707080842760488fe59d37a30","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:34.747042Z","signature_b64":"4X2wbpX925U7tj4i0bV0NgtaP30hmpbZJ1TTc6z4ouGznSBXNj6sEKpgU5uxxCuzsKj1KH1D7sTpYNB88t3PDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d62c3ca33f63d8121d10ae4509156086a8c034f707080842760488fe59d37a30","last_reissued_at":"2026-05-18T03:23:34.746474Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:34.746474Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1104.2830","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":"2026-05-18T03:23:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oDZ1bCMPNfFOyEeuT92203dSO+Sjb7gHGzuZyq47PIKSw69Nn/MTbTsn95pjS+X1lcG9U9OdCI8sttz2R9yfDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:02:59.549411Z"},"content_sha256":"fbd74afc1195f8cb8074a557e9aa21ef6ecca9ef0661a324d68a6c19b06985a4","schema_version":"1.0","event_id":"sha256:fbd74afc1195f8cb8074a557e9aa21ef6ecca9ef0661a324d68a6c19b06985a4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:2YWDZIZ7MPMBEHIQVZCQSFLAQ2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Einstein-Yang-Mills-Chern-Simons solutions in D=2n+1 dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"D. H. Tchrakian, Eugen Radu, Yves Brihaye","submitted_at":"2011-04-14T16:54:55Z","abstract_excerpt":"We investigate finite energy solutions of the Einstein--Yang-Mills--Chern-Simons system in odd spacetime dimensions, D=2n+1, with n>1. Our configurations are static and spherically symmetric, approaching at infinity a Minkowski spacetime background. In contrast with the Abelian case, the contribution of the Chern-Simons term is nontrivial already in the static, spherically symmetric limit. Both globally regular, particle-like solutions and black holes are constructed numerically for several values of D. These solutions carry a nonzero electric charge and have finite mass. For globally regular "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.2830","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":"2026-05-18T03:23:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"14/AUYezGK2eeQNMg4BPFoXBagmOIOGGBl2qdesqunIGpR7WJLIcTfq1Fkri+ATYN+N8QheVkk4LHMZN1rdYCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:02:59.550141Z"},"content_sha256":"7de00f4cff0b35807b1c7a13b23d6424330cbd11cbfb136f359512e116971e8a","schema_version":"1.0","event_id":"sha256:7de00f4cff0b35807b1c7a13b23d6424330cbd11cbfb136f359512e116971e8a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/bundle.json","state_url":"https://pith.science/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/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":"2026-05-30T11:02:59Z","links":{"resolver":"https://pith.science/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2","bundle":"https://pith.science/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/bundle.json","state":"https://pith.science/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2YWDZIZ7MPMBEHIQVZCQSFLAQ2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:2YWDZIZ7MPMBEHIQVZCQSFLAQ2","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":"890ed3092ebd7b32c96d1f879032e89a04b92addb12906bc4bce88b78c9fc22a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-14T16:54:55Z","title_canon_sha256":"431bd525ae8ccc2ce1322f1be1fc878c177836d28aa37fd8f1a072f9e657ae89"},"schema_version":"1.0","source":{"id":"1104.2830","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.2830","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"arxiv_version","alias_value":"1104.2830v2","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.2830","created_at":"2026-05-18T03:23:34Z"},{"alias_kind":"pith_short_12","alias_value":"2YWDZIZ7MPMB","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"2YWDZIZ7MPMBEHIQ","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"2YWDZIZ7","created_at":"2026-05-18T12:26:18Z"}],"graph_snapshots":[{"event_id":"sha256:7de00f4cff0b35807b1c7a13b23d6424330cbd11cbfb136f359512e116971e8a","target":"graph","created_at":"2026-05-18T03:23:34Z","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 finite energy solutions of the Einstein--Yang-Mills--Chern-Simons system in odd spacetime dimensions, D=2n+1, with n>1. Our configurations are static and spherically symmetric, approaching at infinity a Minkowski spacetime background. In contrast with the Abelian case, the contribution of the Chern-Simons term is nontrivial already in the static, spherically symmetric limit. Both globally regular, particle-like solutions and black holes are constructed numerically for several values of D. These solutions carry a nonzero electric charge and have finite mass. For globally regular ","authors_text":"D. H. Tchrakian, Eugen Radu, Yves Brihaye","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-14T16:54:55Z","title":"Einstein-Yang-Mills-Chern-Simons solutions in D=2n+1 dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.2830","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:fbd74afc1195f8cb8074a557e9aa21ef6ecca9ef0661a324d68a6c19b06985a4","target":"record","created_at":"2026-05-18T03:23:34Z","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":"890ed3092ebd7b32c96d1f879032e89a04b92addb12906bc4bce88b78c9fc22a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-04-14T16:54:55Z","title_canon_sha256":"431bd525ae8ccc2ce1322f1be1fc878c177836d28aa37fd8f1a072f9e657ae89"},"schema_version":"1.0","source":{"id":"1104.2830","kind":"arxiv","version":2}},"canonical_sha256":"d62c3ca33f63d8121d10ae4509156086a8c034f707080842760488fe59d37a30","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d62c3ca33f63d8121d10ae4509156086a8c034f707080842760488fe59d37a30","first_computed_at":"2026-05-18T03:23:34.746474Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:34.746474Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4X2wbpX925U7tj4i0bV0NgtaP30hmpbZJ1TTc6z4ouGznSBXNj6sEKpgU5uxxCuzsKj1KH1D7sTpYNB88t3PDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:34.747042Z","signed_message":"canonical_sha256_bytes"},"source_id":"1104.2830","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fbd74afc1195f8cb8074a557e9aa21ef6ecca9ef0661a324d68a6c19b06985a4","sha256:7de00f4cff0b35807b1c7a13b23d6424330cbd11cbfb136f359512e116971e8a"],"state_sha256":"70dd4a09776faab105005ac9fbb70c6b7ead70ad75cda8ba86e71c1a515227a7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c3MRWrEuYvd1r0/Kr+pgQsEvMXpTXPX8W2w0TkikFX5rXO5j4RTKaFMz/HrcMzHRVujIXRbNxG6tjuNFUuYCBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T11:02:59.553388Z","bundle_sha256":"cfb32ddb23cf864019fd10b9165b816cfebaddb3113d9b11215e85ee30466e9d"}}