{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:UTYQ4A5YBBCVTRR57N5SS5TFGD","short_pith_number":"pith:UTYQ4A5Y","canonical_record":{"source":{"id":"1708.02953","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-09T18:01:02Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"53fe9455783b98de8e9611a4863795a8cdd3f77edba81f740b270c4995589ed4","abstract_canon_sha256":"4adb5aaebfd72143694467cd18e79d5ad094e3c8e10c3bd247026a954b25b787"},"schema_version":"1.0"},"canonical_sha256":"a4f10e03b8084559c63dfb7b29766530f24b3465748bf33d2c002f962450a6d0","source":{"kind":"arxiv","id":"1708.02953","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.02953","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"arxiv_version","alias_value":"1708.02953v3","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.02953","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"pith_short_12","alias_value":"UTYQ4A5YBBCV","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"UTYQ4A5YBBCVTRR5","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"UTYQ4A5Y","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:UTYQ4A5YBBCVTRR57N5SS5TFGD","target":"record","payload":{"canonical_record":{"source":{"id":"1708.02953","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-09T18:01:02Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"53fe9455783b98de8e9611a4863795a8cdd3f77edba81f740b270c4995589ed4","abstract_canon_sha256":"4adb5aaebfd72143694467cd18e79d5ad094e3c8e10c3bd247026a954b25b787"},"schema_version":"1.0"},"canonical_sha256":"a4f10e03b8084559c63dfb7b29766530f24b3465748bf33d2c002f962450a6d0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:37.286489Z","signature_b64":"tAKItx5yy12vMLRkGs3k28+OC4QyM0sr36gjnJ3ZNFElBqn5iPyvdGKwQU4w5BAfw7h8RdP8tOOUOr9pfWbTDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a4f10e03b8084559c63dfb7b29766530f24b3465748bf33d2c002f962450a6d0","last_reissued_at":"2026-05-18T00:03:37.285875Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:37.285875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.02953","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:03:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vLsasIjqd5UUDWErmPrIp3lY1SD5txk/hw5vrMjmGi3iWxmf0Rt6nF6/lgHb62jntGHtbds+fZaSV6tPbtYLAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T23:59:11.800062Z"},"content_sha256":"ab13884435aa29183dafe929041fcd6f830be3292e0882c334bb1724ebb00ec4","schema_version":"1.0","event_id":"sha256:ab13884435aa29183dafe929041fcd6f830be3292e0882c334bb1724ebb00ec4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:UTYQ4A5YBBCVTRR57N5SS5TFGD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A rapid holographic phase transition with brane-localized curvature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Barry M. Dillon, Basem Kamal El-Menoufi, Jonathan P. Manuel, Stephan J. Huber","submitted_at":"2017-08-09T18:01:02Z","abstract_excerpt":"We study the finite-temperature properties of the Randall-Sundrum model in the presence of brane-localized curvature. At high temperature, as dictated by AdS/CFT, the theory is in a confined phase dual to the planar AdS black hole. When the radion is stabilized, \\`a la Goldberger-Wise, a holographic first-order phase transition proceeds. The brane-localized curvature contributes to the radion kinetic energy, substantially decreasing the critical bubble energy. Contrary to previous results, the phase transition completes at much larger values of $N$, the number of degrees of freedom in the CFT."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.02953","kind":"arxiv","version":3},"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":"2026-05-18T00:03:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ICDqbjGrKx1I3SdIdoA3QNjQhZqxB/d/Gqo4DSYNzYcbbcQGUI2Asv2D5982yEunz7GDMsF8AFwJnzhbGYD9Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T23:59:11.800794Z"},"content_sha256":"77621cd7ab2809655912b9a6e114e929c19d1037fc8233ec48c6e6415e7aee02","schema_version":"1.0","event_id":"sha256:77621cd7ab2809655912b9a6e114e929c19d1037fc8233ec48c6e6415e7aee02"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/bundle.json","state_url":"https://pith.science/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/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":"2026-05-24T23:59:11Z","links":{"resolver":"https://pith.science/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD","bundle":"https://pith.science/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/bundle.json","state":"https://pith.science/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UTYQ4A5YBBCVTRR57N5SS5TFGD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:UTYQ4A5YBBCVTRR57N5SS5TFGD","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":"4adb5aaebfd72143694467cd18e79d5ad094e3c8e10c3bd247026a954b25b787","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-09T18:01:02Z","title_canon_sha256":"53fe9455783b98de8e9611a4863795a8cdd3f77edba81f740b270c4995589ed4"},"schema_version":"1.0","source":{"id":"1708.02953","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.02953","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"arxiv_version","alias_value":"1708.02953v3","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.02953","created_at":"2026-05-18T00:03:37Z"},{"alias_kind":"pith_short_12","alias_value":"UTYQ4A5YBBCV","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"UTYQ4A5YBBCVTRR5","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"UTYQ4A5Y","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:77621cd7ab2809655912b9a6e114e929c19d1037fc8233ec48c6e6415e7aee02","target":"graph","created_at":"2026-05-18T00:03:37Z","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 study the finite-temperature properties of the Randall-Sundrum model in the presence of brane-localized curvature. At high temperature, as dictated by AdS/CFT, the theory is in a confined phase dual to the planar AdS black hole. When the radion is stabilized, \\`a la Goldberger-Wise, a holographic first-order phase transition proceeds. The brane-localized curvature contributes to the radion kinetic energy, substantially decreasing the critical bubble energy. Contrary to previous results, the phase transition completes at much larger values of $N$, the number of degrees of freedom in the CFT.","authors_text":"Barry M. Dillon, Basem Kamal El-Menoufi, Jonathan P. Manuel, Stephan J. Huber","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-09T18:01:02Z","title":"A rapid holographic phase transition with brane-localized curvature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.02953","kind":"arxiv","version":3},"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:ab13884435aa29183dafe929041fcd6f830be3292e0882c334bb1724ebb00ec4","target":"record","created_at":"2026-05-18T00:03:37Z","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":"4adb5aaebfd72143694467cd18e79d5ad094e3c8e10c3bd247026a954b25b787","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-09T18:01:02Z","title_canon_sha256":"53fe9455783b98de8e9611a4863795a8cdd3f77edba81f740b270c4995589ed4"},"schema_version":"1.0","source":{"id":"1708.02953","kind":"arxiv","version":3}},"canonical_sha256":"a4f10e03b8084559c63dfb7b29766530f24b3465748bf33d2c002f962450a6d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a4f10e03b8084559c63dfb7b29766530f24b3465748bf33d2c002f962450a6d0","first_computed_at":"2026-05-18T00:03:37.285875Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:03:37.285875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tAKItx5yy12vMLRkGs3k28+OC4QyM0sr36gjnJ3ZNFElBqn5iPyvdGKwQU4w5BAfw7h8RdP8tOOUOr9pfWbTDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:03:37.286489Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.02953","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ab13884435aa29183dafe929041fcd6f830be3292e0882c334bb1724ebb00ec4","sha256:77621cd7ab2809655912b9a6e114e929c19d1037fc8233ec48c6e6415e7aee02"],"state_sha256":"c0d416bf9afe86c16561b5c3b8a047c6eb29c011a61814e71276dfe4fba96d0a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fytG2+dRpzB08J//QpmMcPNNBU4cPlDziCMiPIIem5whdzZZaC7SBmBTlx2iEvIKZy3M+wkyWWjT7HInP3sDDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T23:59:11.804025Z","bundle_sha256":"de791df95795c7b87c1a0b9581e5fb140e3cf6bed11247c38d5af5bc1346aeec"}}