{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:W4B2UM4NVESGGR3G5JO64UJ2KY","short_pith_number":"pith:W4B2UM4N","canonical_record":{"source":{"id":"1202.4773","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-21T21:35:10Z","cross_cats_sorted":["astro-ph.HE","hep-ph","hep-th"],"title_canon_sha256":"b275af1f680ba81f12155231668b255202af48da4d4f5e1b3d388c82668d9bd9","abstract_canon_sha256":"48c0a6cf56e2f3c3063e9ffc2ae41b36042017314dcc5f9bd7b679228036db5f"},"schema_version":"1.0"},"canonical_sha256":"b703aa338da924634766ea5dee513a5602ef75a47adb1005322c7c1ed69e6efc","source":{"kind":"arxiv","id":"1202.4773","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4773","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4773v2","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4773","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"pith_short_12","alias_value":"W4B2UM4NVESG","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"W4B2UM4NVESGGR3G","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"W4B2UM4N","created_at":"2026-05-18T12:27:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:W4B2UM4NVESGGR3G5JO64UJ2KY","target":"record","payload":{"canonical_record":{"source":{"id":"1202.4773","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-21T21:35:10Z","cross_cats_sorted":["astro-ph.HE","hep-ph","hep-th"],"title_canon_sha256":"b275af1f680ba81f12155231668b255202af48da4d4f5e1b3d388c82668d9bd9","abstract_canon_sha256":"48c0a6cf56e2f3c3063e9ffc2ae41b36042017314dcc5f9bd7b679228036db5f"},"schema_version":"1.0"},"canonical_sha256":"b703aa338da924634766ea5dee513a5602ef75a47adb1005322c7c1ed69e6efc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:46:45.285765Z","signature_b64":"PIw0JK/DATIQtMP3NkyDKR0buyBvmRGpajBSuiwdP5jx83qkOEJ6lKdynIz0dhTYHi8U21WsHDD4ruiSyyt/Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b703aa338da924634766ea5dee513a5602ef75a47adb1005322c7c1ed69e6efc","last_reissued_at":"2026-05-18T03:46:45.285010Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:46:45.285010Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.4773","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":"2026-05-18T03:46:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B5pWOqpHPB0WTgqpnUWo027FTEqjhpacmAwTomHDRI+9XPq7NSbrbYX2A3M/bJUQKzvjXnF2kJUSVmDyVL60BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:45:55.541819Z"},"content_sha256":"9b6c5c42ccce8a269a2f3ea857bdbf0e37052277cc986b2c276f6f0dc4752e33","schema_version":"1.0","event_id":"sha256:9b6c5c42ccce8a269a2f3ea857bdbf0e37052277cc986b2c276f6f0dc4752e33"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:W4B2UM4NVESGGR3G5JO64UJ2KY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Significance of tension for gravitating masses in Kaluza-Klein models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"Alexander Zhuk, Maxim Eingorn","submitted_at":"2012-02-21T21:35:10Z","abstract_excerpt":"In this letter, we consider the six-dimensional Kaluza-Klein models with spherical compactification of the internal space. Here, we investigate the case of bare gravitating compact objects with the dustlike equation of state $\\hat p_0=0$ in the external (our) space and an arbitrary equation of state $\\hat p_1=\\Omega \\hat\\varepsilon$ in the internal space, where $\\hat \\varepsilon$ is the energy density of the source. This gravitating mass is spherically symmetric in the external space and uniformly smeared over the internal space. In the weak field approximation, the conformal variations of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4773","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":"2026-05-18T03:46:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IUdWECJktet6S+y0g00sI+LjrmT4jP6QgFR2T8Oj76fg3uuBhMWG3eQpvz+yXJPnbr0GrPKYkf9KUrQEQTVYAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:45:55.542512Z"},"content_sha256":"d684c7d1dd9ed2ccab88842731722001c4d0593910292ecb8c81209ba76f639a","schema_version":"1.0","event_id":"sha256:d684c7d1dd9ed2ccab88842731722001c4d0593910292ecb8c81209ba76f639a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/bundle.json","state_url":"https://pith.science/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/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":"2026-05-31T15:45:55Z","links":{"resolver":"https://pith.science/pith/W4B2UM4NVESGGR3G5JO64UJ2KY","bundle":"https://pith.science/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/bundle.json","state":"https://pith.science/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W4B2UM4NVESGGR3G5JO64UJ2KY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:W4B2UM4NVESGGR3G5JO64UJ2KY","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":"48c0a6cf56e2f3c3063e9ffc2ae41b36042017314dcc5f9bd7b679228036db5f","cross_cats_sorted":["astro-ph.HE","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-21T21:35:10Z","title_canon_sha256":"b275af1f680ba81f12155231668b255202af48da4d4f5e1b3d388c82668d9bd9"},"schema_version":"1.0","source":{"id":"1202.4773","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4773","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4773v2","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4773","created_at":"2026-05-18T03:46:45Z"},{"alias_kind":"pith_short_12","alias_value":"W4B2UM4NVESG","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"W4B2UM4NVESGGR3G","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"W4B2UM4N","created_at":"2026-05-18T12:27:25Z"}],"graph_snapshots":[{"event_id":"sha256:d684c7d1dd9ed2ccab88842731722001c4d0593910292ecb8c81209ba76f639a","target":"graph","created_at":"2026-05-18T03:46:45Z","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":"In this letter, we consider the six-dimensional Kaluza-Klein models with spherical compactification of the internal space. Here, we investigate the case of bare gravitating compact objects with the dustlike equation of state $\\hat p_0=0$ in the external (our) space and an arbitrary equation of state $\\hat p_1=\\Omega \\hat\\varepsilon$ in the internal space, where $\\hat \\varepsilon$ is the energy density of the source. This gravitating mass is spherically symmetric in the external space and uniformly smeared over the internal space. In the weak field approximation, the conformal variations of the","authors_text":"Alexander Zhuk, Maxim Eingorn","cross_cats":["astro-ph.HE","hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-21T21:35:10Z","title":"Significance of tension for gravitating masses in Kaluza-Klein models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4773","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":"sha256:9b6c5c42ccce8a269a2f3ea857bdbf0e37052277cc986b2c276f6f0dc4752e33","target":"record","created_at":"2026-05-18T03:46:45Z","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":"48c0a6cf56e2f3c3063e9ffc2ae41b36042017314dcc5f9bd7b679228036db5f","cross_cats_sorted":["astro-ph.HE","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-21T21:35:10Z","title_canon_sha256":"b275af1f680ba81f12155231668b255202af48da4d4f5e1b3d388c82668d9bd9"},"schema_version":"1.0","source":{"id":"1202.4773","kind":"arxiv","version":2}},"canonical_sha256":"b703aa338da924634766ea5dee513a5602ef75a47adb1005322c7c1ed69e6efc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b703aa338da924634766ea5dee513a5602ef75a47adb1005322c7c1ed69e6efc","first_computed_at":"2026-05-18T03:46:45.285010Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:46:45.285010Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PIw0JK/DATIQtMP3NkyDKR0buyBvmRGpajBSuiwdP5jx83qkOEJ6lKdynIz0dhTYHi8U21WsHDD4ruiSyyt/Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:46:45.285765Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.4773","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9b6c5c42ccce8a269a2f3ea857bdbf0e37052277cc986b2c276f6f0dc4752e33","sha256:d684c7d1dd9ed2ccab88842731722001c4d0593910292ecb8c81209ba76f639a"],"state_sha256":"2725627de7d90ce4a6e82ee890c4ea3d7c35d85071ea2ae8a2b77a20279549eb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hi9WosxLnSazX+wF1RxVcKVMbzN1lybmSCuwJzEWL+90iff0Kz4oly2tAxL016osFANnIG7Ziqzo/NQMZJqNBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:45:55.545553Z","bundle_sha256":"5120aafa39733ab0363431bd755247e2dc16a31e9769dad4584aa025c1694c87"}}