{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:5RCOTOQUUI52SXZKYIS7XPQJZ7","short_pith_number":"pith:5RCOTOQU","canonical_record":{"source":{"id":"1306.2384","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-06-10T23:34:08Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"b31a08e1e7421f61e23a16993efab87d4c95f6f3f0795262089b4a77fa0efc1c","abstract_canon_sha256":"d0a76e4161471a531353fe7b79c7fb472e6187ff738cf4199337f295a05d9dd3"},"schema_version":"1.0"},"canonical_sha256":"ec44e9ba14a23ba95f2ac225fbbe09cfc456a72836274b7fb2c0662e485be4a6","source":{"kind":"arxiv","id":"1306.2384","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.2384","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"arxiv_version","alias_value":"1306.2384v3","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.2384","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"pith_short_12","alias_value":"5RCOTOQUUI52","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5RCOTOQUUI52SXZK","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5RCOTOQU","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:5RCOTOQUUI52SXZKYIS7XPQJZ7","target":"record","payload":{"canonical_record":{"source":{"id":"1306.2384","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-06-10T23:34:08Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"b31a08e1e7421f61e23a16993efab87d4c95f6f3f0795262089b4a77fa0efc1c","abstract_canon_sha256":"d0a76e4161471a531353fe7b79c7fb472e6187ff738cf4199337f295a05d9dd3"},"schema_version":"1.0"},"canonical_sha256":"ec44e9ba14a23ba95f2ac225fbbe09cfc456a72836274b7fb2c0662e485be4a6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:11:35.624507Z","signature_b64":"tIl7qd53RMwvbih8JvNwc+Rfgij4TclkMJfsCQuvlhvLGTMfd/yvdydzn1pnkfG+6bn8XwDyahqC6kVH5FngBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec44e9ba14a23ba95f2ac225fbbe09cfc456a72836274b7fb2c0662e485be4a6","last_reissued_at":"2026-05-18T03:11:35.623794Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:11:35.623794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.2384","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":"2026-05-18T03:11:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c5RGFs5xwQjYcQYXfkiR2dfXP8ceVoxePeRjyqA0E+7mm5BGEHulZOgkjyHS69d5Qk1ISCz/0Br9hwoJn/8HDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:52:40.087942Z"},"content_sha256":"8d956a694f2d8b9a1c182212dda3e1fe60fa0ffc1e656d582b8f64a23242876b","schema_version":"1.0","event_id":"sha256:8d956a694f2d8b9a1c182212dda3e1fe60fa0ffc1e656d582b8f64a23242876b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:5RCOTOQUUI52SXZKYIS7XPQJZ7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rare decay B -> K ll form factors from lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Chris Bouchard, Christopher Monahan, G. Peter Lepage, Heechang Na, Junko Shigemitsu","submitted_at":"2013-06-10T23:34:08Z","abstract_excerpt":"We calculate, for the first time using unquenched lattice QCD, form factors for the rare decay B -> Kll in and beyond the Standard Model. Our lattice QCD calculation utilizes a nonrelativistic QCD formulation for the b valence quarks, the highly improved staggered quark formulation for the light valence quarks, and employs the MILC 2+1 asqtad ensembles. The form factor results, based on the z expansion, are valid over the full kinematic range of q^2. We construct the ratios f0/f+ and fT/f+, which are useful in constraining new physics and verifying effective theory form factor symmetry relatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.2384","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":"2026-05-18T03:11:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4qNXXrX0XROCLoueo86f1evizRnapEfLTV2TDVHrNR6rw8xOnvsr19Kc7D8PSxNojx3Nn0SerSOQhml2/O4nAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:52:40.088519Z"},"content_sha256":"922391c2e804a20d04936bac9a5ea2688f62aff1d3123ca0b2609ad9ee88a9e6","schema_version":"1.0","event_id":"sha256:922391c2e804a20d04936bac9a5ea2688f62aff1d3123ca0b2609ad9ee88a9e6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/bundle.json","state_url":"https://pith.science/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/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":"2026-05-27T21:52:40Z","links":{"resolver":"https://pith.science/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7","bundle":"https://pith.science/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/bundle.json","state":"https://pith.science/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5RCOTOQUUI52SXZKYIS7XPQJZ7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:5RCOTOQUUI52SXZKYIS7XPQJZ7","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":"d0a76e4161471a531353fe7b79c7fb472e6187ff738cf4199337f295a05d9dd3","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-06-10T23:34:08Z","title_canon_sha256":"b31a08e1e7421f61e23a16993efab87d4c95f6f3f0795262089b4a77fa0efc1c"},"schema_version":"1.0","source":{"id":"1306.2384","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.2384","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"arxiv_version","alias_value":"1306.2384v3","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.2384","created_at":"2026-05-18T03:11:35Z"},{"alias_kind":"pith_short_12","alias_value":"5RCOTOQUUI52","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5RCOTOQUUI52SXZK","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5RCOTOQU","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:922391c2e804a20d04936bac9a5ea2688f62aff1d3123ca0b2609ad9ee88a9e6","target":"graph","created_at":"2026-05-18T03:11:35Z","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 calculate, for the first time using unquenched lattice QCD, form factors for the rare decay B -> Kll in and beyond the Standard Model. Our lattice QCD calculation utilizes a nonrelativistic QCD formulation for the b valence quarks, the highly improved staggered quark formulation for the light valence quarks, and employs the MILC 2+1 asqtad ensembles. The form factor results, based on the z expansion, are valid over the full kinematic range of q^2. We construct the ratios f0/f+ and fT/f+, which are useful in constraining new physics and verifying effective theory form factor symmetry relatio","authors_text":"Chris Bouchard, Christopher Monahan, G. Peter Lepage, Heechang Na, Junko Shigemitsu","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-06-10T23:34:08Z","title":"Rare decay B -> K ll form factors from lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.2384","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":"sha256:8d956a694f2d8b9a1c182212dda3e1fe60fa0ffc1e656d582b8f64a23242876b","target":"record","created_at":"2026-05-18T03:11:35Z","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":"d0a76e4161471a531353fe7b79c7fb472e6187ff738cf4199337f295a05d9dd3","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-06-10T23:34:08Z","title_canon_sha256":"b31a08e1e7421f61e23a16993efab87d4c95f6f3f0795262089b4a77fa0efc1c"},"schema_version":"1.0","source":{"id":"1306.2384","kind":"arxiv","version":3}},"canonical_sha256":"ec44e9ba14a23ba95f2ac225fbbe09cfc456a72836274b7fb2c0662e485be4a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ec44e9ba14a23ba95f2ac225fbbe09cfc456a72836274b7fb2c0662e485be4a6","first_computed_at":"2026-05-18T03:11:35.623794Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:11:35.623794Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tIl7qd53RMwvbih8JvNwc+Rfgij4TclkMJfsCQuvlhvLGTMfd/yvdydzn1pnkfG+6bn8XwDyahqC6kVH5FngBg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:11:35.624507Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.2384","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8d956a694f2d8b9a1c182212dda3e1fe60fa0ffc1e656d582b8f64a23242876b","sha256:922391c2e804a20d04936bac9a5ea2688f62aff1d3123ca0b2609ad9ee88a9e6"],"state_sha256":"a4c5ab828e472026699073820e2de26eac100fc4070fcacc779725671be91383"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s8OVZ0ajWp/aceH7DsLats4qonOhe7/8MjpQuwIOCdMFz3EaCLcpdLI5E+J/QaLcg2j7PCujo+83yDACpaVvDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:52:40.091261Z","bundle_sha256":"0939338d965130eec0295282720ef742ef0c23166f1618c0ab56c11877239d6c"}}