{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:XV5EIKCH33XMHSJPTGWCLVTGTR","short_pith_number":"pith:XV5EIKCH","canonical_record":{"source":{"id":"gr-qc/0211081","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2002-11-25T13:09:27Z","cross_cats_sorted":[],"title_canon_sha256":"2cad45e356287780d170d91cbdf9b741e49cfc0d4437b238b09fc781ba32783c","abstract_canon_sha256":"ab3ae75bcd78283e01ed01275ffc4a5fa8b5f168b8d872ae3b51196a512ee91d"},"schema_version":"1.0"},"canonical_sha256":"bd7a442847deeec3c92f99ac25d6669c7cf949b17a0b5cd91411bcb1f47f3cf8","source":{"kind":"arxiv","id":"gr-qc/0211081","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/0211081","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0211081v1","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0211081","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"XV5EIKCH33XM","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_16","alias_value":"XV5EIKCH33XMHSJP","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_8","alias_value":"XV5EIKCH","created_at":"2026-07-04T16:33:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:XV5EIKCH33XMHSJPTGWCLVTGTR","target":"record","payload":{"canonical_record":{"source":{"id":"gr-qc/0211081","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2002-11-25T13:09:27Z","cross_cats_sorted":[],"title_canon_sha256":"2cad45e356287780d170d91cbdf9b741e49cfc0d4437b238b09fc781ba32783c","abstract_canon_sha256":"ab3ae75bcd78283e01ed01275ffc4a5fa8b5f168b8d872ae3b51196a512ee91d"},"schema_version":"1.0"},"canonical_sha256":"bd7a442847deeec3c92f99ac25d6669c7cf949b17a0b5cd91411bcb1f47f3cf8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:33:48.399255Z","signature_b64":"IjHH9DWqMMqW6yk5YSXVR07ruGgKkYlMjq9noSIXYiVyT/MsewGZYq4caD6I9nExe6DrYnAaV22tR3GxhqKGAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd7a442847deeec3c92f99ac25d6669c7cf949b17a0b5cd91411bcb1f47f3cf8","last_reissued_at":"2026-07-04T16:33:48.398912Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:33:48.398912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"gr-qc/0211081","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":"2026-07-04T16:33:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tCCyplJ0Ua7AyN1L0LZ/rE4JJRS17kVI3DE7JVqs45SvXWEBEa5aQrWuM189jYXRETggd5sN4aZ7GguEqyqSAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T00:57:44.344214Z"},"content_sha256":"6b7aecdbc950cc951d5a88abd122fb3ec0ec5ecf2dcf80644d340639a05decfc","schema_version":"1.0","event_id":"sha256:6b7aecdbc950cc951d5a88abd122fb3ec0ec5ecf2dcf80644d340639a05decfc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:XV5EIKCH33XMHSJPTGWCLVTGTR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thick domain wall spacetimes with and without reflection symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Alejandra Melfo, Aureliano Skirzewski, Nelson Pantoja","submitted_at":"2002-11-25T13:09:27Z","abstract_excerpt":"We show that the spacetimes of domain wall solutions to the coupled Einstein-scalar field equations with a given scalar field potential fall into two classes, depending on whether or not reflection symmetry on the wall is imposed. Solutions with reflection symmetry are dynamic, while the asymmetric ones are static. Asymmetric walls are asymptotically flat on one side and reduce to the Taub spacetime on the other. Examples of asymmetric thick walls in D-dimensional spacetimes are given, and results on the thin-wall limit of the dynamic, symmetric walls are extended to the asymmetric case. The p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0211081","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/gr-qc/0211081/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":"2026-07-04T16:33:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WuWTkvu8ntf300dGqOj38GxcpyDzIHJrDQ8Tpz2Z6f96j9Apxb9w5mFjwYyTTxh2mdaFwDgwLlJ/XPE1t7o9BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-20T00:57:44.344746Z"},"content_sha256":"99d9479219f6b552e77e08e6c431b4ae6bcf8f0a7952e6512b07e2b28a804cf6","schema_version":"1.0","event_id":"sha256:99d9479219f6b552e77e08e6c431b4ae6bcf8f0a7952e6512b07e2b28a804cf6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/bundle.json","state_url":"https://pith.science/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/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":"2026-08-20T00:57:44Z","links":{"resolver":"https://pith.science/pith/XV5EIKCH33XMHSJPTGWCLVTGTR","bundle":"https://pith.science/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/bundle.json","state":"https://pith.science/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XV5EIKCH33XMHSJPTGWCLVTGTR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:XV5EIKCH33XMHSJPTGWCLVTGTR","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":"ab3ae75bcd78283e01ed01275ffc4a5fa8b5f168b8d872ae3b51196a512ee91d","cross_cats_sorted":[],"license":"","primary_cat":"gr-qc","submitted_at":"2002-11-25T13:09:27Z","title_canon_sha256":"2cad45e356287780d170d91cbdf9b741e49cfc0d4437b238b09fc781ba32783c"},"schema_version":"1.0","source":{"id":"gr-qc/0211081","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/0211081","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0211081v1","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0211081","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_12","alias_value":"XV5EIKCH33XM","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_16","alias_value":"XV5EIKCH33XMHSJP","created_at":"2026-07-04T16:33:48Z"},{"alias_kind":"pith_short_8","alias_value":"XV5EIKCH","created_at":"2026-07-04T16:33:48Z"}],"graph_snapshots":[{"event_id":"sha256:99d9479219f6b552e77e08e6c431b4ae6bcf8f0a7952e6512b07e2b28a804cf6","target":"graph","created_at":"2026-07-04T16:33:48Z","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/gr-qc/0211081/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show that the spacetimes of domain wall solutions to the coupled Einstein-scalar field equations with a given scalar field potential fall into two classes, depending on whether or not reflection symmetry on the wall is imposed. Solutions with reflection symmetry are dynamic, while the asymmetric ones are static. Asymmetric walls are asymptotically flat on one side and reduce to the Taub spacetime on the other. Examples of asymmetric thick walls in D-dimensional spacetimes are given, and results on the thin-wall limit of the dynamic, symmetric walls are extended to the asymmetric case. The p","authors_text":"Alejandra Melfo, Aureliano Skirzewski, Nelson Pantoja","cross_cats":[],"headline":"","license":"","primary_cat":"gr-qc","submitted_at":"2002-11-25T13:09:27Z","title":"Thick domain wall spacetimes with and without reflection symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0211081","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":"sha256:6b7aecdbc950cc951d5a88abd122fb3ec0ec5ecf2dcf80644d340639a05decfc","target":"record","created_at":"2026-07-04T16:33:48Z","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":"ab3ae75bcd78283e01ed01275ffc4a5fa8b5f168b8d872ae3b51196a512ee91d","cross_cats_sorted":[],"license":"","primary_cat":"gr-qc","submitted_at":"2002-11-25T13:09:27Z","title_canon_sha256":"2cad45e356287780d170d91cbdf9b741e49cfc0d4437b238b09fc781ba32783c"},"schema_version":"1.0","source":{"id":"gr-qc/0211081","kind":"arxiv","version":1}},"canonical_sha256":"bd7a442847deeec3c92f99ac25d6669c7cf949b17a0b5cd91411bcb1f47f3cf8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bd7a442847deeec3c92f99ac25d6669c7cf949b17a0b5cd91411bcb1f47f3cf8","first_computed_at":"2026-07-04T16:33:48.398912Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:33:48.398912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IjHH9DWqMMqW6yk5YSXVR07ruGgKkYlMjq9noSIXYiVyT/MsewGZYq4caD6I9nExe6DrYnAaV22tR3GxhqKGAw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:33:48.399255Z","signed_message":"canonical_sha256_bytes"},"source_id":"gr-qc/0211081","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6b7aecdbc950cc951d5a88abd122fb3ec0ec5ecf2dcf80644d340639a05decfc","sha256:99d9479219f6b552e77e08e6c431b4ae6bcf8f0a7952e6512b07e2b28a804cf6"],"state_sha256":"ebe352b048f66401831ba97a939216f3478b8aad632378ce3434aafb3ff6399c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oH+zxGMNMw5Ps50xauYeBBIEcPwOGDSrh2h3T+WjyR2396id+rhkbcW0LwMtySS7D2m0Y2qlnwfN7ZluHEjqCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-20T00:57:44.347198Z","bundle_sha256":"22915e4e6dd3c128f88b1ea3885cdb16c7b3a33b9e88f178cb194f5db6bcf41c"}}