{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:VPOE3OPMABDADSAUOJVRRZWE4Z","short_pith_number":"pith:VPOE3OPM","canonical_record":{"source":{"id":"0907.1952","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-07-11T09:37:56Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"b919312f7ce4aa2ad4b3835264380dea4a3916ca546380c02849e4d37db9117a","abstract_canon_sha256":"5e9c1676ea87408cb89291cdff5b9aee4af28058e4d72f40668391037f263f9a"},"schema_version":"1.0"},"canonical_sha256":"abdc4db9ec004601c814726b18e6c4e667abbd603276f051376aab42018ba244","source":{"kind":"arxiv","id":"0907.1952","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0907.1952","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"arxiv_version","alias_value":"0907.1952v3","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0907.1952","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"pith_short_12","alias_value":"VPOE3OPMABDA","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"VPOE3OPMABDADSAU","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"VPOE3OPM","created_at":"2026-05-18T12:26:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:VPOE3OPMABDADSAUOJVRRZWE4Z","target":"record","payload":{"canonical_record":{"source":{"id":"0907.1952","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-07-11T09:37:56Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"b919312f7ce4aa2ad4b3835264380dea4a3916ca546380c02849e4d37db9117a","abstract_canon_sha256":"5e9c1676ea87408cb89291cdff5b9aee4af28058e4d72f40668391037f263f9a"},"schema_version":"1.0"},"canonical_sha256":"abdc4db9ec004601c814726b18e6c4e667abbd603276f051376aab42018ba244","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:38.862770Z","signature_b64":"nHOLLUEg8e6eNCV++k86VRtdq1kVAvfEPfrlRNX4XBafb5CajsOLQYBOb1drlz3ElnCoili/fAvzR39D3PFmBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"abdc4db9ec004601c814726b18e6c4e667abbd603276f051376aab42018ba244","last_reissued_at":"2026-05-18T02:34:38.862301Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:38.862301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0907.1952","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":"2026-05-18T02:34:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9hpwGGkh1FxzTSxSKe7c1nPo+Qw2+XvjnYu6ODM+2/hZ35oEfCAcGMR3GUtYOcGEs/I4qEP5djTxZL9Ilf6aCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:38:30.027488Z"},"content_sha256":"17cc0d2438b63145dc2adfe6649375d93c0d0a4b53ee1906b42e51e4625ba1dd","schema_version":"1.0","event_id":"sha256:17cc0d2438b63145dc2adfe6649375d93c0d0a4b53ee1906b42e51e4625ba1dd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:VPOE3OPMABDADSAUOJVRRZWE4Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scalar-Kinetic Branes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Ke Yang, Yuan Zhong, Yu-Xiao Liu","submitted_at":"2009-07-11T09:37:56Z","abstract_excerpt":"This work tries to find out thick brane solutions in braneworld scenarios described by a real scalar field in the presence of a scalar-kinetic term $F(X,\\phi)=X\\phi^m$ with a single extra dimension, where $X=\\frac12\\nabla_M\\phi\\nabla^M\\phi$ stands for the standard kinetic term and $m=0,1,2\\cdots$. We mainly consider bent branes, namely de Sitter and Anti-de Sitter four-dimensional slices. The solutions of a flat brane are obtained when taking the four-dimensional cosmological constant $\\Lambda_4\\rightarrow 0$. When the parameter $m=0$, these solutions turn to those of the standard scenario. Th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0907.1952","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":"2026-05-18T02:34:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c1Z736ghjQB+RisiDfVmsCLATe4orB1oPwEGx76MNO6Z4k2hL078egDjyEwnf/SAHrzcs0XuMe52Ke+ZJrmKBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:38:30.027940Z"},"content_sha256":"9eae37b9ac8c5a916f96a8321df222dbc1dfc864e1a14a8608207fdc7bf1d663","schema_version":"1.0","event_id":"sha256:9eae37b9ac8c5a916f96a8321df222dbc1dfc864e1a14a8608207fdc7bf1d663"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/bundle.json","state_url":"https://pith.science/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/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":"2026-05-27T20:38:30Z","links":{"resolver":"https://pith.science/pith/VPOE3OPMABDADSAUOJVRRZWE4Z","bundle":"https://pith.science/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/bundle.json","state":"https://pith.science/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VPOE3OPMABDADSAUOJVRRZWE4Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:VPOE3OPMABDADSAUOJVRRZWE4Z","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":"5e9c1676ea87408cb89291cdff5b9aee4af28058e4d72f40668391037f263f9a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-07-11T09:37:56Z","title_canon_sha256":"b919312f7ce4aa2ad4b3835264380dea4a3916ca546380c02849e4d37db9117a"},"schema_version":"1.0","source":{"id":"0907.1952","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0907.1952","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"arxiv_version","alias_value":"0907.1952v3","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0907.1952","created_at":"2026-05-18T02:34:38Z"},{"alias_kind":"pith_short_12","alias_value":"VPOE3OPMABDA","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"VPOE3OPMABDADSAU","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"VPOE3OPM","created_at":"2026-05-18T12:26:02Z"}],"graph_snapshots":[{"event_id":"sha256:9eae37b9ac8c5a916f96a8321df222dbc1dfc864e1a14a8608207fdc7bf1d663","target":"graph","created_at":"2026-05-18T02:34:38Z","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":"This work tries to find out thick brane solutions in braneworld scenarios described by a real scalar field in the presence of a scalar-kinetic term $F(X,\\phi)=X\\phi^m$ with a single extra dimension, where $X=\\frac12\\nabla_M\\phi\\nabla^M\\phi$ stands for the standard kinetic term and $m=0,1,2\\cdots$. We mainly consider bent branes, namely de Sitter and Anti-de Sitter four-dimensional slices. The solutions of a flat brane are obtained when taking the four-dimensional cosmological constant $\\Lambda_4\\rightarrow 0$. When the parameter $m=0$, these solutions turn to those of the standard scenario. Th","authors_text":"Ke Yang, Yuan Zhong, Yu-Xiao Liu","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-07-11T09:37:56Z","title":"Scalar-Kinetic Branes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0907.1952","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":"sha256:17cc0d2438b63145dc2adfe6649375d93c0d0a4b53ee1906b42e51e4625ba1dd","target":"record","created_at":"2026-05-18T02:34:38Z","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":"5e9c1676ea87408cb89291cdff5b9aee4af28058e4d72f40668391037f263f9a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-07-11T09:37:56Z","title_canon_sha256":"b919312f7ce4aa2ad4b3835264380dea4a3916ca546380c02849e4d37db9117a"},"schema_version":"1.0","source":{"id":"0907.1952","kind":"arxiv","version":3}},"canonical_sha256":"abdc4db9ec004601c814726b18e6c4e667abbd603276f051376aab42018ba244","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"abdc4db9ec004601c814726b18e6c4e667abbd603276f051376aab42018ba244","first_computed_at":"2026-05-18T02:34:38.862301Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:34:38.862301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nHOLLUEg8e6eNCV++k86VRtdq1kVAvfEPfrlRNX4XBafb5CajsOLQYBOb1drlz3ElnCoili/fAvzR39D3PFmBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:34:38.862770Z","signed_message":"canonical_sha256_bytes"},"source_id":"0907.1952","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:17cc0d2438b63145dc2adfe6649375d93c0d0a4b53ee1906b42e51e4625ba1dd","sha256:9eae37b9ac8c5a916f96a8321df222dbc1dfc864e1a14a8608207fdc7bf1d663"],"state_sha256":"aa205b6553b73ff586c1068ac9fb5e4b92cc79feda53d6cc85fb8592b5931ac5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"geDM3C3U7ZD/GcApOrh05Jf6HQmRvwgaaGWe6McNhByZn+DKBlvAtNalbL+xY3HybSbJ3ldTev/BwZlnnaTADw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T20:38:30.031250Z","bundle_sha256":"6a931336f326b273c74dc9ff101461c41a7701bd34b9a4ae1ae810d0ec3f5dff"}}