{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:2TRNGRFV6YHP27SNQRAQCRY54P","short_pith_number":"pith:2TRNGRFV","canonical_record":{"source":{"id":"1402.6147","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-25T12:21:13Z","cross_cats_sorted":["gr-qc","math-ph","math.MP","nlin.SI"],"title_canon_sha256":"51af9dece46b56bffa9a5b147c3d340728d40bc35fb3d1dd213aed05cbbe749c","abstract_canon_sha256":"d1b970f6cfb49b4bb84c5b3b25faa19889e17d9bbbed3dc7764406b5d2a5029f"},"schema_version":"1.0"},"canonical_sha256":"d4e2d344b5f60efd7e4d844101471de3cf18d2bd3e17fdb94f0a9b2bd39f818c","source":{"kind":"arxiv","id":"1402.6147","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.6147","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"arxiv_version","alias_value":"1402.6147v2","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6147","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"pith_short_12","alias_value":"2TRNGRFV6YHP","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2TRNGRFV6YHP27SN","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2TRNGRFV","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:2TRNGRFV6YHP27SNQRAQCRY54P","target":"record","payload":{"canonical_record":{"source":{"id":"1402.6147","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-25T12:21:13Z","cross_cats_sorted":["gr-qc","math-ph","math.MP","nlin.SI"],"title_canon_sha256":"51af9dece46b56bffa9a5b147c3d340728d40bc35fb3d1dd213aed05cbbe749c","abstract_canon_sha256":"d1b970f6cfb49b4bb84c5b3b25faa19889e17d9bbbed3dc7764406b5d2a5029f"},"schema_version":"1.0"},"canonical_sha256":"d4e2d344b5f60efd7e4d844101471de3cf18d2bd3e17fdb94f0a9b2bd39f818c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:28.545275Z","signature_b64":"jPI8tN4zmRYUhonJr3Giivn7vPqCnv1Uj5bi6TN8xvP9FNny6mk5b9jkLmZtq56KVanImd0KRvymvND6wQ6HDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4e2d344b5f60efd7e4d844101471de3cf18d2bd3e17fdb94f0a9b2bd39f818c","last_reissued_at":"2026-05-18T01:44:28.544780Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:28.544780Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.6147","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":"2026-05-18T01:44:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OHwIVl+usgBT92K+KIVozehMOWA35KMRaAYCVKwD8s4t8iH+gNuSAKw7yWCLTlePn4L5vzqYBKcXdNJUzqbyBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:37:28.918300Z"},"content_sha256":"e18c30a2c25f1f80e189b55d35e189ef87e82a4129c2836d0d105c09ada6c768","schema_version":"1.0","event_id":"sha256:e18c30a2c25f1f80e189b55d35e189ef87e82a4129c2836d0d105c09ada6c768"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:2TRNGRFV6YHP27SNQRAQCRY54P","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Jordanian deformation of AdS space in type IIB supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","math-ph","math.MP","nlin.SI"],"primary_cat":"hep-th","authors_text":"Io Kawaguchi, Kentaroh Yoshida, Takuya Matsumoto","submitted_at":"2014-02-25T12:21:13Z","abstract_excerpt":"We consider a Jordanian deformation of the AdS_5xS^5 superstring action by taking a simple R-operator which satisfies the classical Yang-Baxter equation. The metric and NS-NS two-form are explicitly derived with a coordinate system. Only the AdS part is deformed and the resulting geometry contains the 3D Schrodinger spacetime as a subspace. Then we present the full solution in type IIB supergravity by determining the other field components. In particular, the dilaton is constant and a R-R three-form field strength is turned on. The symmetry of the solution is [SL(2,R)xU(1)^2] x [SU(3)xU(1)] an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6147","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":"2026-05-18T01:44:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LIKIo8SVl3LrepfqOIDVv0LTF6Bnk0I8asxnvjmc+TX07A3HVDR2ld18lBYFINZLo0TJEPBRuiuxFe0VErVVAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:37:28.918984Z"},"content_sha256":"14fac0ab486f672b69f2868984674be55dd1f190954100eda298eadb4c75244c","schema_version":"1.0","event_id":"sha256:14fac0ab486f672b69f2868984674be55dd1f190954100eda298eadb4c75244c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2TRNGRFV6YHP27SNQRAQCRY54P/bundle.json","state_url":"https://pith.science/pith/2TRNGRFV6YHP27SNQRAQCRY54P/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2TRNGRFV6YHP27SNQRAQCRY54P/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":"2026-05-27T02:37:28Z","links":{"resolver":"https://pith.science/pith/2TRNGRFV6YHP27SNQRAQCRY54P","bundle":"https://pith.science/pith/2TRNGRFV6YHP27SNQRAQCRY54P/bundle.json","state":"https://pith.science/pith/2TRNGRFV6YHP27SNQRAQCRY54P/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2TRNGRFV6YHP27SNQRAQCRY54P/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2TRNGRFV6YHP27SNQRAQCRY54P","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":"d1b970f6cfb49b4bb84c5b3b25faa19889e17d9bbbed3dc7764406b5d2a5029f","cross_cats_sorted":["gr-qc","math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-25T12:21:13Z","title_canon_sha256":"51af9dece46b56bffa9a5b147c3d340728d40bc35fb3d1dd213aed05cbbe749c"},"schema_version":"1.0","source":{"id":"1402.6147","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.6147","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"arxiv_version","alias_value":"1402.6147v2","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6147","created_at":"2026-05-18T01:44:28Z"},{"alias_kind":"pith_short_12","alias_value":"2TRNGRFV6YHP","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2TRNGRFV6YHP27SN","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2TRNGRFV","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:14fac0ab486f672b69f2868984674be55dd1f190954100eda298eadb4c75244c","target":"graph","created_at":"2026-05-18T01:44:28Z","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 consider a Jordanian deformation of the AdS_5xS^5 superstring action by taking a simple R-operator which satisfies the classical Yang-Baxter equation. The metric and NS-NS two-form are explicitly derived with a coordinate system. Only the AdS part is deformed and the resulting geometry contains the 3D Schrodinger spacetime as a subspace. Then we present the full solution in type IIB supergravity by determining the other field components. In particular, the dilaton is constant and a R-R three-form field strength is turned on. The symmetry of the solution is [SL(2,R)xU(1)^2] x [SU(3)xU(1)] an","authors_text":"Io Kawaguchi, Kentaroh Yoshida, Takuya Matsumoto","cross_cats":["gr-qc","math-ph","math.MP","nlin.SI"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-25T12:21:13Z","title":"A Jordanian deformation of AdS space in type IIB supergravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6147","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:e18c30a2c25f1f80e189b55d35e189ef87e82a4129c2836d0d105c09ada6c768","target":"record","created_at":"2026-05-18T01:44:28Z","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":"d1b970f6cfb49b4bb84c5b3b25faa19889e17d9bbbed3dc7764406b5d2a5029f","cross_cats_sorted":["gr-qc","math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-25T12:21:13Z","title_canon_sha256":"51af9dece46b56bffa9a5b147c3d340728d40bc35fb3d1dd213aed05cbbe749c"},"schema_version":"1.0","source":{"id":"1402.6147","kind":"arxiv","version":2}},"canonical_sha256":"d4e2d344b5f60efd7e4d844101471de3cf18d2bd3e17fdb94f0a9b2bd39f818c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d4e2d344b5f60efd7e4d844101471de3cf18d2bd3e17fdb94f0a9b2bd39f818c","first_computed_at":"2026-05-18T01:44:28.544780Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:44:28.544780Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jPI8tN4zmRYUhonJr3Giivn7vPqCnv1Uj5bi6TN8xvP9FNny6mk5b9jkLmZtq56KVanImd0KRvymvND6wQ6HDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:44:28.545275Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.6147","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e18c30a2c25f1f80e189b55d35e189ef87e82a4129c2836d0d105c09ada6c768","sha256:14fac0ab486f672b69f2868984674be55dd1f190954100eda298eadb4c75244c"],"state_sha256":"4bc3770c6045d269d966e43fc766f5192a02a4ab4eff0b14b6e6656e77ea707b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S2ftlFA9o/pFpgoahLQKeN0YP8rFDGjJllDyooYcs+uGr5brfQ6zKnoL3Q6YCCQFgCwhJG8Ty/O5gE/TF7tDBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T02:37:28.922293Z","bundle_sha256":"d244cc0150be9991d0146fa951f0779130a958a132d43b20a10387717613efb2"}}