{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:ZL7OAJR3QXWRUDX6AVNKFEMEEZ","short_pith_number":"pith:ZL7OAJR3","canonical_record":{"source":{"id":"1410.5090","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-19T16:44:49Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3beb3380d02309472a3eebd1538fc4ded78d86cd61bd58430f79306d649f860d","abstract_canon_sha256":"61fcdf54c36adf6501cefa7d324ea132b88af939bf1d7fdf96b9cc5e2b8fdb8d"},"schema_version":"1.0"},"canonical_sha256":"cafee0263b85ed1a0efe055aa291842658237e0c2f7261d1bc86f506ec77eb7a","source":{"kind":"arxiv","id":"1410.5090","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.5090","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"arxiv_version","alias_value":"1410.5090v2","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.5090","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"pith_short_12","alias_value":"ZL7OAJR3QXWR","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZL7OAJR3QXWRUDX6","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZL7OAJR3","created_at":"2026-05-18T12:28:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:ZL7OAJR3QXWRUDX6AVNKFEMEEZ","target":"record","payload":{"canonical_record":{"source":{"id":"1410.5090","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-19T16:44:49Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3beb3380d02309472a3eebd1538fc4ded78d86cd61bd58430f79306d649f860d","abstract_canon_sha256":"61fcdf54c36adf6501cefa7d324ea132b88af939bf1d7fdf96b9cc5e2b8fdb8d"},"schema_version":"1.0"},"canonical_sha256":"cafee0263b85ed1a0efe055aa291842658237e0c2f7261d1bc86f506ec77eb7a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:43.698665Z","signature_b64":"lHXGxQoRrksednKpLUpWqA1YEXsCXtTOG9rh/c888DQiFcXfkaEUzJoQmt43OCLtpKpR7RMfCCNsjjG3x+jVCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cafee0263b85ed1a0efe055aa291842658237e0c2f7261d1bc86f506ec77eb7a","last_reissued_at":"2026-05-18T01:41:43.698188Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:43.698188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.5090","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":"2026-05-18T01:41:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Btw0leX+HMWBzw7g42Na2HZGau5F6pRWW3D6OYpNRWPBL6U3NfGP8eB9XcsooHTji7a4vs1XcBUFs4u+4GsnAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T11:25:47.642561Z"},"content_sha256":"99410102da65bb5683161ae36a682fab7c9ae066dfea6b6452483630adfaa48d","schema_version":"1.0","event_id":"sha256:99410102da65bb5683161ae36a682fab7c9ae066dfea6b6452483630adfaa48d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:ZL7OAJR3QXWRUDX6AVNKFEMEEZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An SO(3)$\\times$SO(3) invariant solution of $D=11$ supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Hadi Godazgar, Hermann Nicolai, Krzysztof Pilch, Mahdi Godazgar, Olaf Krueger","submitted_at":"2014-10-19T16:44:49Z","abstract_excerpt":"We construct a new SO(3)$\\times$SO(3) invariant non-supersymmetric solution of the bosonic field equations of $D=11$ supergravity from the corresponding stationary point of maximal gauged $N=8$ supergravity by making use of the non-linear uplift formulae for the metric and the 3-form potential. The latter are crucial as this solution appears to be inaccessible to traditional techniques of solving Einstein's field equations, and is arguably the most complicated closed form solution of this type ever found. The solution is also a promising candidate for a stable non-supersymmetric solution of M-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.5090","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":"2026-05-18T01:41:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dsO1RAC/mGFSOET3V1bJksAoi74gkeup38bL4DkFRqebw7tAO6b3PXO84cZvQ0z56NUWTjCP4lK3GR5IPMTaBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T11:25:47.643133Z"},"content_sha256":"225bbd937c5fb95f4aec0d29a162d41fbdf10d8981eb535baa3dcef7f454fc50","schema_version":"1.0","event_id":"sha256:225bbd937c5fb95f4aec0d29a162d41fbdf10d8981eb535baa3dcef7f454fc50"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/bundle.json","state_url":"https://pith.science/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/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":"2026-06-01T11:25:47Z","links":{"resolver":"https://pith.science/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ","bundle":"https://pith.science/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/bundle.json","state":"https://pith.science/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZL7OAJR3QXWRUDX6AVNKFEMEEZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:ZL7OAJR3QXWRUDX6AVNKFEMEEZ","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":"61fcdf54c36adf6501cefa7d324ea132b88af939bf1d7fdf96b9cc5e2b8fdb8d","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-19T16:44:49Z","title_canon_sha256":"3beb3380d02309472a3eebd1538fc4ded78d86cd61bd58430f79306d649f860d"},"schema_version":"1.0","source":{"id":"1410.5090","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.5090","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"arxiv_version","alias_value":"1410.5090v2","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.5090","created_at":"2026-05-18T01:41:43Z"},{"alias_kind":"pith_short_12","alias_value":"ZL7OAJR3QXWR","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZL7OAJR3QXWRUDX6","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZL7OAJR3","created_at":"2026-05-18T12:28:59Z"}],"graph_snapshots":[{"event_id":"sha256:225bbd937c5fb95f4aec0d29a162d41fbdf10d8981eb535baa3dcef7f454fc50","target":"graph","created_at":"2026-05-18T01:41:43Z","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 construct a new SO(3)$\\times$SO(3) invariant non-supersymmetric solution of the bosonic field equations of $D=11$ supergravity from the corresponding stationary point of maximal gauged $N=8$ supergravity by making use of the non-linear uplift formulae for the metric and the 3-form potential. The latter are crucial as this solution appears to be inaccessible to traditional techniques of solving Einstein's field equations, and is arguably the most complicated closed form solution of this type ever found. The solution is also a promising candidate for a stable non-supersymmetric solution of M-","authors_text":"Hadi Godazgar, Hermann Nicolai, Krzysztof Pilch, Mahdi Godazgar, Olaf Krueger","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-19T16:44:49Z","title":"An SO(3)$\\times$SO(3) invariant solution of $D=11$ supergravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.5090","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":"sha256:99410102da65bb5683161ae36a682fab7c9ae066dfea6b6452483630adfaa48d","target":"record","created_at":"2026-05-18T01:41:43Z","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":"61fcdf54c36adf6501cefa7d324ea132b88af939bf1d7fdf96b9cc5e2b8fdb8d","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-10-19T16:44:49Z","title_canon_sha256":"3beb3380d02309472a3eebd1538fc4ded78d86cd61bd58430f79306d649f860d"},"schema_version":"1.0","source":{"id":"1410.5090","kind":"arxiv","version":2}},"canonical_sha256":"cafee0263b85ed1a0efe055aa291842658237e0c2f7261d1bc86f506ec77eb7a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cafee0263b85ed1a0efe055aa291842658237e0c2f7261d1bc86f506ec77eb7a","first_computed_at":"2026-05-18T01:41:43.698188Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:43.698188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lHXGxQoRrksednKpLUpWqA1YEXsCXtTOG9rh/c888DQiFcXfkaEUzJoQmt43OCLtpKpR7RMfCCNsjjG3x+jVCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:43.698665Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.5090","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:99410102da65bb5683161ae36a682fab7c9ae066dfea6b6452483630adfaa48d","sha256:225bbd937c5fb95f4aec0d29a162d41fbdf10d8981eb535baa3dcef7f454fc50"],"state_sha256":"eecbe87a3e486d76edda3370a5df0ded4a73dec860b1fb1e49c0250743e0cadb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CGNAYL5VzQnoy3NwnvgROJYADJKOOHWthQ2KMymxsfBx6xUVs2SHcXlTP+xyWDzXRGe8IeJk+3UvIwMiRljHCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T11:25:47.645663Z","bundle_sha256":"e7631b725270589a0f3cba688653018691200ca2bf0652d96c2af0d7f98803a8"}}