{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:JXZPLLSL462XD3IQ7SXFUUO6ZF","short_pith_number":"pith:JXZPLLSL","canonical_record":{"source":{"id":"2306.00328","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2023-06-01T04:14:56Z","cross_cats_sorted":[],"title_canon_sha256":"82d8bb9c8965226e3873818d1e2e4ba1200df7cf0860b05c9dac3d9c48f0e3e1","abstract_canon_sha256":"7c0a288f6eeaf68d336caf1d1f079e0db77bd191ef408a8b73871243f52b0bcf"},"schema_version":"1.0"},"canonical_sha256":"4df2f5ae4be7b571ed10fcae5a51dec97db35ed6d251b428976fe30ab1321e50","source":{"kind":"arxiv","id":"2306.00328","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.00328","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"arxiv_version","alias_value":"2306.00328v1","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.00328","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_12","alias_value":"JXZPLLSL462X","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_16","alias_value":"JXZPLLSL462XD3IQ","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_8","alias_value":"JXZPLLSL","created_at":"2026-07-05T06:16:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:JXZPLLSL462XD3IQ7SXFUUO6ZF","target":"record","payload":{"canonical_record":{"source":{"id":"2306.00328","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2023-06-01T04:14:56Z","cross_cats_sorted":[],"title_canon_sha256":"82d8bb9c8965226e3873818d1e2e4ba1200df7cf0860b05c9dac3d9c48f0e3e1","abstract_canon_sha256":"7c0a288f6eeaf68d336caf1d1f079e0db77bd191ef408a8b73871243f52b0bcf"},"schema_version":"1.0"},"canonical_sha256":"4df2f5ae4be7b571ed10fcae5a51dec97db35ed6d251b428976fe30ab1321e50","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:16:25.015639Z","signature_b64":"PHtQHDemKcEQcne4LkIHWZZG1ybhGqvzRPuFF/utxcId3h80F/kd88lxRVv9lvwYf69K9Xd1LAtQmmSk4bP4CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4df2f5ae4be7b571ed10fcae5a51dec97db35ed6d251b428976fe30ab1321e50","last_reissued_at":"2026-07-05T06:16:25.015146Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:16:25.015146Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2306.00328","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:16:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LkwUOzlYyOXg1YsXDhAPBu3gyY6tWxLLB86H0jmpBdzFR7h6eT2KVuLUVmuBnVKxHDDsgj426uqysrT0bL5aBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T02:47:52.713628Z"},"content_sha256":"23c8b09147806e2b44ddf16d6370b3c0cca1ec3513a3fc3a12e6e07afc5ac4cb","schema_version":"1.0","event_id":"sha256:23c8b09147806e2b44ddf16d6370b3c0cca1ec3513a3fc3a12e6e07afc5ac4cb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:JXZPLLSL462XD3IQ7SXFUUO6ZF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charged Anisotropic Models with Complexity-free Condition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Sharif, Tayyab Naseer","submitted_at":"2023-06-01T04:14:56Z","abstract_excerpt":"This paper uses the definition of complexity for a static spherically symmetric spacetime and extends it to the case of charged distribution. We formulate the Einstein-Maxwell field equations corresponding to the anisotropic interior and calculate two different mass functions. We then take Reissner-Nordstr\\\"{o}m metric as an exterior spacetime to find the matching conditions at the spherical boundary. Some scalars are developed from the orthogonal splitting of the curvature tensor, and we call one of them, i.e., $\\mathcal{Y}_{TF}$ as the complexity factor for the considered setup. Further, the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.00328","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2306.00328/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T06:16:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5vQtjad175Pl8NEg0X/UdSLU4kYyD2gWf7SFmJcVn34czV4eowlGMnNLuCKh2OXToVC30a42rlX2HgRduQFnCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T02:47:52.714040Z"},"content_sha256":"39c67112c3dd81e90753f9cccc3cf09039d4736f04b1263d70ddb1b52d2c0a65","schema_version":"1.0","event_id":"sha256:39c67112c3dd81e90753f9cccc3cf09039d4736f04b1263d70ddb1b52d2c0a65"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/bundle.json","state_url":"https://pith.science/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/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":"2026-07-09T02:47:52Z","links":{"resolver":"https://pith.science/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF","bundle":"https://pith.science/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/bundle.json","state":"https://pith.science/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JXZPLLSL462XD3IQ7SXFUUO6ZF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:JXZPLLSL462XD3IQ7SXFUUO6ZF","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":"7c0a288f6eeaf68d336caf1d1f079e0db77bd191ef408a8b73871243f52b0bcf","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2023-06-01T04:14:56Z","title_canon_sha256":"82d8bb9c8965226e3873818d1e2e4ba1200df7cf0860b05c9dac3d9c48f0e3e1"},"schema_version":"1.0","source":{"id":"2306.00328","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.00328","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"arxiv_version","alias_value":"2306.00328v1","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.00328","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_12","alias_value":"JXZPLLSL462X","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_16","alias_value":"JXZPLLSL462XD3IQ","created_at":"2026-07-05T06:16:25Z"},{"alias_kind":"pith_short_8","alias_value":"JXZPLLSL","created_at":"2026-07-05T06:16:25Z"}],"graph_snapshots":[{"event_id":"sha256:39c67112c3dd81e90753f9cccc3cf09039d4736f04b1263d70ddb1b52d2c0a65","target":"graph","created_at":"2026-07-05T06:16:25Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2306.00328/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"This paper uses the definition of complexity for a static spherically symmetric spacetime and extends it to the case of charged distribution. We formulate the Einstein-Maxwell field equations corresponding to the anisotropic interior and calculate two different mass functions. We then take Reissner-Nordstr\\\"{o}m metric as an exterior spacetime to find the matching conditions at the spherical boundary. Some scalars are developed from the orthogonal splitting of the curvature tensor, and we call one of them, i.e., $\\mathcal{Y}_{TF}$ as the complexity factor for the considered setup. Further, the","authors_text":"M. Sharif, Tayyab Naseer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2023-06-01T04:14:56Z","title":"Charged Anisotropic Models with Complexity-free Condition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.00328","kind":"arxiv","version":1},"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":"sha256:23c8b09147806e2b44ddf16d6370b3c0cca1ec3513a3fc3a12e6e07afc5ac4cb","target":"record","created_at":"2026-07-05T06:16:25Z","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":"7c0a288f6eeaf68d336caf1d1f079e0db77bd191ef408a8b73871243f52b0bcf","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2023-06-01T04:14:56Z","title_canon_sha256":"82d8bb9c8965226e3873818d1e2e4ba1200df7cf0860b05c9dac3d9c48f0e3e1"},"schema_version":"1.0","source":{"id":"2306.00328","kind":"arxiv","version":1}},"canonical_sha256":"4df2f5ae4be7b571ed10fcae5a51dec97db35ed6d251b428976fe30ab1321e50","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4df2f5ae4be7b571ed10fcae5a51dec97db35ed6d251b428976fe30ab1321e50","first_computed_at":"2026-07-05T06:16:25.015146Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:16:25.015146Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PHtQHDemKcEQcne4LkIHWZZG1ybhGqvzRPuFF/utxcId3h80F/kd88lxRVv9lvwYf69K9Xd1LAtQmmSk4bP4CA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:16:25.015639Z","signed_message":"canonical_sha256_bytes"},"source_id":"2306.00328","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:23c8b09147806e2b44ddf16d6370b3c0cca1ec3513a3fc3a12e6e07afc5ac4cb","sha256:39c67112c3dd81e90753f9cccc3cf09039d4736f04b1263d70ddb1b52d2c0a65"],"state_sha256":"76611b9f7201f4af7c3e1678b6771fd0fe0b92747296e40e2d34c6b0963673f6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C8ImMS2exdePiDz1BGyUsXH0CPG3qCAz5PXFNEx4PRe7w5h2Gx/gTQKvf76P2yv2/emDUx6hpL1PcgrNwzmQAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-09T02:47:52.716225Z","bundle_sha256":"8a176c0b3d27f26fc5f0b3b179f4654505031f1074f14fe6a3e9d5b30764b151"}}