{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:3K5WILUV76YOTWULZTK42CJYL4","short_pith_number":"pith:3K5WILUV","canonical_record":{"source":{"id":"1109.0528","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-09-02T19:35:18Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3f17688e21124fbb54d1eb3803401ef4acdec5c8465636e6d3419ddcbd200d93","abstract_canon_sha256":"aceb70004c6d4ee9c40fdea03fbe85645e4499dba315b54aa40bd70dd5cccb73"},"schema_version":"1.0"},"canonical_sha256":"dabb642e95ffb0e9da8bccd5cd09385f1d6b7665d598368dcbec743e8f7a30d5","source":{"kind":"arxiv","id":"1109.0528","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.0528","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"arxiv_version","alias_value":"1109.0528v4","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.0528","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"pith_short_12","alias_value":"3K5WILUV76YO","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"3K5WILUV76YOTWUL","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"3K5WILUV","created_at":"2026-05-18T12:26:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:3K5WILUV76YOTWULZTK42CJYL4","target":"record","payload":{"canonical_record":{"source":{"id":"1109.0528","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-09-02T19:35:18Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3f17688e21124fbb54d1eb3803401ef4acdec5c8465636e6d3419ddcbd200d93","abstract_canon_sha256":"aceb70004c6d4ee9c40fdea03fbe85645e4499dba315b54aa40bd70dd5cccb73"},"schema_version":"1.0"},"canonical_sha256":"dabb642e95ffb0e9da8bccd5cd09385f1d6b7665d598368dcbec743e8f7a30d5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:01:50.915857Z","signature_b64":"AlhHXPSIQWB8SljnlSvH3M9zYTWl4H3ilP7RntDrbYvGAwUcu33ylhu8bMczhciHoUcE1RsIqleTb/xFPq7gCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dabb642e95ffb0e9da8bccd5cd09385f1d6b7665d598368dcbec743e8f7a30d5","last_reissued_at":"2026-05-18T04:01:50.915366Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:01:50.915366Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1109.0528","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:01:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ki7yb8dbQsgC0gzM6bFlIuHi4FLnaT5p0A+ia6w8KpNmrlov5diHIrOFvE8nfXXH6AKpPme8B5F69GAzqYrNDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T10:31:41.871797Z"},"content_sha256":"d128c455d3c541b9e0f5711fa6bbf1369aae661de3c888b1adb972724e482f16","schema_version":"1.0","event_id":"sha256:d128c455d3c541b9e0f5711fa6bbf1369aae661de3c888b1adb972724e482f16"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:3K5WILUV76YOTWULZTK42CJYL4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Static Anisotropic Solutions in f(T) Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"physics.gen-ph","authors_text":"Manuel E. Rodrigues, M. Hamani Daouda, M. J. S. Houndjo","submitted_at":"2011-09-02T19:35:18Z","abstract_excerpt":"In a previously work, we undertook a static and anisotropic content in $f(T)$ theory and obtained new spherically symmetric solutions considering a constant torsion and some particular conditions for the pressure. In this paper, still in the framework of $f(T)$ theory, new spherically symmetric solutions are obtained, first considering the general case of an isotropic fluid and later the anisotropic content case in which the generalized conditions for the matter content are considered such that the energy density, the radial and tangential pressures depend on the algebraic $f(T)$ and its deriv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.0528","kind":"arxiv","version":4},"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":"2026-05-18T04:01:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sJq1ljauSKJHcxo6CGVhfQPsVHIFW5Qn10mmuY9cCjm5nWhbZ7gZCvfycc8bQAqh2W2EW3s2EhkY7aBfECQFBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T10:31:41.872140Z"},"content_sha256":"c39609226081073ba8a4561acf0f56b0781e171f3a8b08a3524377749c87c942","schema_version":"1.0","event_id":"sha256:c39609226081073ba8a4561acf0f56b0781e171f3a8b08a3524377749c87c942"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3K5WILUV76YOTWULZTK42CJYL4/bundle.json","state_url":"https://pith.science/pith/3K5WILUV76YOTWULZTK42CJYL4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3K5WILUV76YOTWULZTK42CJYL4/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":"2026-05-28T10:31:41Z","links":{"resolver":"https://pith.science/pith/3K5WILUV76YOTWULZTK42CJYL4","bundle":"https://pith.science/pith/3K5WILUV76YOTWULZTK42CJYL4/bundle.json","state":"https://pith.science/pith/3K5WILUV76YOTWULZTK42CJYL4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3K5WILUV76YOTWULZTK42CJYL4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:3K5WILUV76YOTWULZTK42CJYL4","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":"aceb70004c6d4ee9c40fdea03fbe85645e4499dba315b54aa40bd70dd5cccb73","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-09-02T19:35:18Z","title_canon_sha256":"3f17688e21124fbb54d1eb3803401ef4acdec5c8465636e6d3419ddcbd200d93"},"schema_version":"1.0","source":{"id":"1109.0528","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.0528","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"arxiv_version","alias_value":"1109.0528v4","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.0528","created_at":"2026-05-18T04:01:50Z"},{"alias_kind":"pith_short_12","alias_value":"3K5WILUV76YO","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"3K5WILUV76YOTWUL","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"3K5WILUV","created_at":"2026-05-18T12:26:18Z"}],"graph_snapshots":[{"event_id":"sha256:c39609226081073ba8a4561acf0f56b0781e171f3a8b08a3524377749c87c942","target":"graph","created_at":"2026-05-18T04:01:50Z","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":"In a previously work, we undertook a static and anisotropic content in $f(T)$ theory and obtained new spherically symmetric solutions considering a constant torsion and some particular conditions for the pressure. In this paper, still in the framework of $f(T)$ theory, new spherically symmetric solutions are obtained, first considering the general case of an isotropic fluid and later the anisotropic content case in which the generalized conditions for the matter content are considered such that the energy density, the radial and tangential pressures depend on the algebraic $f(T)$ and its deriv","authors_text":"Manuel E. Rodrigues, M. Hamani Daouda, M. J. S. Houndjo","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-09-02T19:35:18Z","title":"Static Anisotropic Solutions in f(T) Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.0528","kind":"arxiv","version":4},"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:d128c455d3c541b9e0f5711fa6bbf1369aae661de3c888b1adb972724e482f16","target":"record","created_at":"2026-05-18T04:01:50Z","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":"aceb70004c6d4ee9c40fdea03fbe85645e4499dba315b54aa40bd70dd5cccb73","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2011-09-02T19:35:18Z","title_canon_sha256":"3f17688e21124fbb54d1eb3803401ef4acdec5c8465636e6d3419ddcbd200d93"},"schema_version":"1.0","source":{"id":"1109.0528","kind":"arxiv","version":4}},"canonical_sha256":"dabb642e95ffb0e9da8bccd5cd09385f1d6b7665d598368dcbec743e8f7a30d5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dabb642e95ffb0e9da8bccd5cd09385f1d6b7665d598368dcbec743e8f7a30d5","first_computed_at":"2026-05-18T04:01:50.915366Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:01:50.915366Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AlhHXPSIQWB8SljnlSvH3M9zYTWl4H3ilP7RntDrbYvGAwUcu33ylhu8bMczhciHoUcE1RsIqleTb/xFPq7gCw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:01:50.915857Z","signed_message":"canonical_sha256_bytes"},"source_id":"1109.0528","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d128c455d3c541b9e0f5711fa6bbf1369aae661de3c888b1adb972724e482f16","sha256:c39609226081073ba8a4561acf0f56b0781e171f3a8b08a3524377749c87c942"],"state_sha256":"b9d8532bafc473179470c023dcf00311981097446cbbb4bc57dea67da54a7ad6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7rfE/hKQ/KXQgilXJUJJ01WRQDhkqim6hDel+YpxoCrRR8rIZHQv4vSsPkQCg3ELNyrtnGu5Zstmyuxj5YD1Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T10:31:41.874107Z","bundle_sha256":"7c9df9420492863d8ff48284fa02b525c2a8f049d5d0c8d6a6901e16974455e7"}}