{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:6Q6FUNXRWIS23K4RPW6QB76SAJ","short_pith_number":"pith:6Q6FUNXR","canonical_record":{"source":{"id":"1511.04344","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-11-13T16:33:12Z","cross_cats_sorted":["hep-th","physics.comp-ph"],"title_canon_sha256":"6363f508cb560c090dd6e317204df14dd8640ea72b4f5cb7e46b8fd757e14e34","abstract_canon_sha256":"915355b8a7d9a14530b9f4a35c11587511c973e17b80a76fea88be8512692102"},"schema_version":"1.0"},"canonical_sha256":"f43c5a36f1b225adab917dbd00ffd20261b3dc6bd4df6a8e07b90ad12f220b82","source":{"kind":"arxiv","id":"1511.04344","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.04344","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"arxiv_version","alias_value":"1511.04344v2","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.04344","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"pith_short_12","alias_value":"6Q6FUNXRWIS2","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6Q6FUNXRWIS23K4R","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6Q6FUNXR","created_at":"2026-05-18T12:29:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:6Q6FUNXRWIS23K4RPW6QB76SAJ","target":"record","payload":{"canonical_record":{"source":{"id":"1511.04344","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-11-13T16:33:12Z","cross_cats_sorted":["hep-th","physics.comp-ph"],"title_canon_sha256":"6363f508cb560c090dd6e317204df14dd8640ea72b4f5cb7e46b8fd757e14e34","abstract_canon_sha256":"915355b8a7d9a14530b9f4a35c11587511c973e17b80a76fea88be8512692102"},"schema_version":"1.0"},"canonical_sha256":"f43c5a36f1b225adab917dbd00ffd20261b3dc6bd4df6a8e07b90ad12f220b82","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:41.657677Z","signature_b64":"btjp3BthbctJhy+7BU1OY1Qv83tRiqfzy2meUeTaEFGmFZDg6eEDAZFOKCg6cqaFVlHLUM2Xz6muR/nBdSxKCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f43c5a36f1b225adab917dbd00ffd20261b3dc6bd4df6a8e07b90ad12f220b82","last_reissued_at":"2026-05-18T01:21:41.657090Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:41.657090Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1511.04344","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":"2026-05-18T01:21:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XMpan3VmEP8sOWY6XGGHLj4RlROUfsRMfl35cJRcKcneEdZhqPj3QlbQjNNBQ95e5y1XV2ey8qPShHcIt5QwAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T00:24:11.204688Z"},"content_sha256":"1a7cf8b3ff62ad900d1a538bd18867d1e40b2d25585a51a98e1976e4738a4bda","schema_version":"1.0","event_id":"sha256:1a7cf8b3ff62ad900d1a538bd18867d1e40b2d25585a51a98e1976e4738a4bda"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:6Q6FUNXRWIS23K4RPW6QB76SAJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New Features of Gravitational Collapse in Anti-de Sitter Spacetimes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","physics.comp-ph"],"primary_cat":"gr-qc","authors_text":"Carlos F. Sopuerta, Daniel Santos-Oliv\\'an","submitted_at":"2015-11-13T16:33:12Z","abstract_excerpt":"Gravitational collapse of a massless scalar field in spherically symmetric anti-de Sitter (AdS) spacetimes presents a new phenomenology with a series of critical points whose dynamics is discretely self-similar as in the asymptotically flat case. Each critical point is the limit of a branch of scalar field configurations that have bounced off the AdS boundary a fixed number of times before forming an apparent horizon. We present results from a numerical study that focus on the interfaces between branches. We find that there is a mass gap between branches and that subcritical configurations nea"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.04344","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":"2026-05-18T01:21:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3cS/jRC7UakeHJwr+gn/Nz/8DG9NLmBj//PyMDEKQ+/b/K0YwBtGinYilrBdrtp1v38hRLD4D366e5yxL8DfAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T00:24:11.205030Z"},"content_sha256":"e44d347a337662d169e37e8648e95b83ed6f98afb9856c934074e9215e00203b","schema_version":"1.0","event_id":"sha256:e44d347a337662d169e37e8648e95b83ed6f98afb9856c934074e9215e00203b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/bundle.json","state_url":"https://pith.science/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/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":"2026-06-09T00:24:11Z","links":{"resolver":"https://pith.science/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ","bundle":"https://pith.science/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/bundle.json","state":"https://pith.science/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6Q6FUNXRWIS23K4RPW6QB76SAJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:6Q6FUNXRWIS23K4RPW6QB76SAJ","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":"915355b8a7d9a14530b9f4a35c11587511c973e17b80a76fea88be8512692102","cross_cats_sorted":["hep-th","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-11-13T16:33:12Z","title_canon_sha256":"6363f508cb560c090dd6e317204df14dd8640ea72b4f5cb7e46b8fd757e14e34"},"schema_version":"1.0","source":{"id":"1511.04344","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.04344","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"arxiv_version","alias_value":"1511.04344v2","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.04344","created_at":"2026-05-18T01:21:41Z"},{"alias_kind":"pith_short_12","alias_value":"6Q6FUNXRWIS2","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6Q6FUNXRWIS23K4R","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6Q6FUNXR","created_at":"2026-05-18T12:29:07Z"}],"graph_snapshots":[{"event_id":"sha256:e44d347a337662d169e37e8648e95b83ed6f98afb9856c934074e9215e00203b","target":"graph","created_at":"2026-05-18T01:21:41Z","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":"Gravitational collapse of a massless scalar field in spherically symmetric anti-de Sitter (AdS) spacetimes presents a new phenomenology with a series of critical points whose dynamics is discretely self-similar as in the asymptotically flat case. Each critical point is the limit of a branch of scalar field configurations that have bounced off the AdS boundary a fixed number of times before forming an apparent horizon. We present results from a numerical study that focus on the interfaces between branches. We find that there is a mass gap between branches and that subcritical configurations nea","authors_text":"Carlos F. Sopuerta, Daniel Santos-Oliv\\'an","cross_cats":["hep-th","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-11-13T16:33:12Z","title":"New Features of Gravitational Collapse in Anti-de Sitter Spacetimes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.04344","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":"sha256:1a7cf8b3ff62ad900d1a538bd18867d1e40b2d25585a51a98e1976e4738a4bda","target":"record","created_at":"2026-05-18T01:21:41Z","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":"915355b8a7d9a14530b9f4a35c11587511c973e17b80a76fea88be8512692102","cross_cats_sorted":["hep-th","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-11-13T16:33:12Z","title_canon_sha256":"6363f508cb560c090dd6e317204df14dd8640ea72b4f5cb7e46b8fd757e14e34"},"schema_version":"1.0","source":{"id":"1511.04344","kind":"arxiv","version":2}},"canonical_sha256":"f43c5a36f1b225adab917dbd00ffd20261b3dc6bd4df6a8e07b90ad12f220b82","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f43c5a36f1b225adab917dbd00ffd20261b3dc6bd4df6a8e07b90ad12f220b82","first_computed_at":"2026-05-18T01:21:41.657090Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:21:41.657090Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"btjp3BthbctJhy+7BU1OY1Qv83tRiqfzy2meUeTaEFGmFZDg6eEDAZFOKCg6cqaFVlHLUM2Xz6muR/nBdSxKCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:21:41.657677Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.04344","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1a7cf8b3ff62ad900d1a538bd18867d1e40b2d25585a51a98e1976e4738a4bda","sha256:e44d347a337662d169e37e8648e95b83ed6f98afb9856c934074e9215e00203b"],"state_sha256":"88797e8aa81b5f32b080d17705a74fd417ea0fd4e1914c7fb13c16252ca70a47"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Mnx39afH5/GTMHlFrBHcxUey+bFs8nUGANCnjKaqlWcks8lpLkKuYX19PnWECHDg80ykuQAHFH68zTUtCCYhAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T00:24:11.206836Z","bundle_sha256":"846394ee5d532d96bcb6a9a29f8b894d75828c9b8cda73a291bc56d66d4e504b"}}