{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:KROCKHML4KBRVLDQAVCUXLONUX","short_pith_number":"pith:KROCKHML","canonical_record":{"source":{"id":"hep-th/0309071","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-09-07T04:45:16Z","cross_cats_sorted":[],"title_canon_sha256":"7e1e4c660ebdb217f1d8c1d1aad20d55e44419706f56d0e1415f9fe04dc88ee6","abstract_canon_sha256":"248fac445f6e087435fe61a174541916beca1df5c0f65a86da1d39e5bd030bd1"},"schema_version":"1.0"},"canonical_sha256":"545c251d8be2831aac7005454badcda5dde38a86ec3da1825aa06bac81dffe5a","source":{"kind":"arxiv","id":"hep-th/0309071","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0309071","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0309071v1","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0309071","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"pith_short_12","alias_value":"KROCKHML4KBR","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"KROCKHML4KBRVLDQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"KROCKHML","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:KROCKHML4KBRVLDQAVCUXLONUX","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0309071","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-09-07T04:45:16Z","cross_cats_sorted":[],"title_canon_sha256":"7e1e4c660ebdb217f1d8c1d1aad20d55e44419706f56d0e1415f9fe04dc88ee6","abstract_canon_sha256":"248fac445f6e087435fe61a174541916beca1df5c0f65a86da1d39e5bd030bd1"},"schema_version":"1.0"},"canonical_sha256":"545c251d8be2831aac7005454badcda5dde38a86ec3da1825aa06bac81dffe5a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:46.692288Z","signature_b64":"vdWJKi8PWDZ4RsQRqIVkWgxZeRNdNGLkBiC4sr7Zf7Rmg9DMRlCGaKhKuqqhwGrz3axdyW7uxpo0a+Wjzpq0AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"545c251d8be2831aac7005454badcda5dde38a86ec3da1825aa06bac81dffe5a","last_reissued_at":"2026-05-18T01:38:46.691863Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:46.691863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0309071","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":"2026-05-18T01:38:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PPvPzTIHacIK5icjvOlufBlUxWUPQ4SWjQxig4eJcdeKMH124wsmOSlezD71SKTN3IriY/ksaYslLSP7Y7leBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T12:35:52.112988Z"},"content_sha256":"f4643f535d2971dde2c00769e19ba0e13ec4265e53b4b6fd8c415b395b8687d3","schema_version":"1.0","event_id":"sha256:f4643f535d2971dde2c00769e19ba0e13ec4265e53b4b6fd8c415b395b8687d3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:KROCKHML4KBRVLDQAVCUXLONUX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Newton Law in DGP Brane-World with Semi-Infinite Extra Dimension","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. K. Park, S. Tamaryan, Yan-Gang Miao","submitted_at":"2003-09-07T04:45:16Z","abstract_excerpt":"Newton potential for DGP brane-world scenario is examined when the extra dimension is semi-infinite. The final form of the potential involves a self-adjoint extension parameter $\\alpha$, which plays a role of an additional mass (or distance) scale. The striking feature of Newton potential in this setup is that the potential behaves as seven-dimensional in long range when $\\alpha$ is nonzero. For small $\\alpha$ there is an intermediate range where the potential is five-dimensional. Five-dimensional Newton constant decreases with increase of $\\alpha$ from zero. In the short range the four-dimens"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0309071","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":""},"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":"2026-05-18T01:38:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gmtFVXud6Dd6jYTPVoMPXj8VFxBc4J0o/6kcT9LEhGYG12VYmZAdv74fYHaxLoIxemjvthBAfgleEfZCEr5aCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T12:35:52.113647Z"},"content_sha256":"b177768fc7f3ce6baccd992028d479742c013d4c6b193674cad574cdca49d7cd","schema_version":"1.0","event_id":"sha256:b177768fc7f3ce6baccd992028d479742c013d4c6b193674cad574cdca49d7cd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KROCKHML4KBRVLDQAVCUXLONUX/bundle.json","state_url":"https://pith.science/pith/KROCKHML4KBRVLDQAVCUXLONUX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KROCKHML4KBRVLDQAVCUXLONUX/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":"2026-06-06T12:35:52Z","links":{"resolver":"https://pith.science/pith/KROCKHML4KBRVLDQAVCUXLONUX","bundle":"https://pith.science/pith/KROCKHML4KBRVLDQAVCUXLONUX/bundle.json","state":"https://pith.science/pith/KROCKHML4KBRVLDQAVCUXLONUX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KROCKHML4KBRVLDQAVCUXLONUX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:KROCKHML4KBRVLDQAVCUXLONUX","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":"248fac445f6e087435fe61a174541916beca1df5c0f65a86da1d39e5bd030bd1","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-09-07T04:45:16Z","title_canon_sha256":"7e1e4c660ebdb217f1d8c1d1aad20d55e44419706f56d0e1415f9fe04dc88ee6"},"schema_version":"1.0","source":{"id":"hep-th/0309071","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0309071","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0309071v1","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0309071","created_at":"2026-05-18T01:38:46Z"},{"alias_kind":"pith_short_12","alias_value":"KROCKHML4KBR","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"KROCKHML4KBRVLDQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"KROCKHML","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:b177768fc7f3ce6baccd992028d479742c013d4c6b193674cad574cdca49d7cd","target":"graph","created_at":"2026-05-18T01:38:46Z","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":"Newton potential for DGP brane-world scenario is examined when the extra dimension is semi-infinite. The final form of the potential involves a self-adjoint extension parameter $\\alpha$, which plays a role of an additional mass (or distance) scale. The striking feature of Newton potential in this setup is that the potential behaves as seven-dimensional in long range when $\\alpha$ is nonzero. For small $\\alpha$ there is an intermediate range where the potential is five-dimensional. Five-dimensional Newton constant decreases with increase of $\\alpha$ from zero. In the short range the four-dimens","authors_text":"D. K. Park, S. Tamaryan, Yan-Gang Miao","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-09-07T04:45:16Z","title":"Newton Law in DGP Brane-World with Semi-Infinite Extra Dimension"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0309071","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:f4643f535d2971dde2c00769e19ba0e13ec4265e53b4b6fd8c415b395b8687d3","target":"record","created_at":"2026-05-18T01:38:46Z","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":"248fac445f6e087435fe61a174541916beca1df5c0f65a86da1d39e5bd030bd1","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-09-07T04:45:16Z","title_canon_sha256":"7e1e4c660ebdb217f1d8c1d1aad20d55e44419706f56d0e1415f9fe04dc88ee6"},"schema_version":"1.0","source":{"id":"hep-th/0309071","kind":"arxiv","version":1}},"canonical_sha256":"545c251d8be2831aac7005454badcda5dde38a86ec3da1825aa06bac81dffe5a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"545c251d8be2831aac7005454badcda5dde38a86ec3da1825aa06bac81dffe5a","first_computed_at":"2026-05-18T01:38:46.691863Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:46.691863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vdWJKi8PWDZ4RsQRqIVkWgxZeRNdNGLkBiC4sr7Zf7Rmg9DMRlCGaKhKuqqhwGrz3axdyW7uxpo0a+Wjzpq0AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:46.692288Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0309071","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f4643f535d2971dde2c00769e19ba0e13ec4265e53b4b6fd8c415b395b8687d3","sha256:b177768fc7f3ce6baccd992028d479742c013d4c6b193674cad574cdca49d7cd"],"state_sha256":"34a6dd7c67863d019b459dca1e02ee91b9b68e9797e42e12c26fb6c5828d8032"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vk4W22NVrCFaIB47YhmfT1EmY3QApFU/DEag1cynF8b2+qC/8fRH21ORI+krcb8YB79TbfdSVcQ4KCrlQXd1Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T12:35:52.117698Z","bundle_sha256":"9bbb41cdf1fb2e8f7fe2788ba15aca62c16bf4cb91ffd43cd7d472515dd6b863"}}