{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:PISA6BFWVBWQ25YKAKTIYPLLZQ","short_pith_number":"pith:PISA6BFW","canonical_record":{"source":{"id":"1509.08113","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-27T17:36:45Z","cross_cats_sorted":[],"title_canon_sha256":"e9aab299e33a30b4a8e0aa9d9f5d193fcffa82cd119d9f228dd271bd1638bc25","abstract_canon_sha256":"e4c922eb0f8a406ad233a54f324e1e2acc07acf92736a47c85db244646d33ad9"},"schema_version":"1.0"},"canonical_sha256":"7a240f04b6a86d0d770a02a68c3d6bcc1f5d62393bc253257fad4b9a9ba3cf5a","source":{"kind":"arxiv","id":"1509.08113","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08113","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08113v1","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08113","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"pith_short_12","alias_value":"PISA6BFWVBWQ","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"PISA6BFWVBWQ25YK","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"PISA6BFW","created_at":"2026-05-18T12:29:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:PISA6BFWVBWQ25YKAKTIYPLLZQ","target":"record","payload":{"canonical_record":{"source":{"id":"1509.08113","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-27T17:36:45Z","cross_cats_sorted":[],"title_canon_sha256":"e9aab299e33a30b4a8e0aa9d9f5d193fcffa82cd119d9f228dd271bd1638bc25","abstract_canon_sha256":"e4c922eb0f8a406ad233a54f324e1e2acc07acf92736a47c85db244646d33ad9"},"schema_version":"1.0"},"canonical_sha256":"7a240f04b6a86d0d770a02a68c3d6bcc1f5d62393bc253257fad4b9a9ba3cf5a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:09.481416Z","signature_b64":"sJRmMfD6zHoXjDZ/dw8Emf1Y0HjJV7xbT7vbl0bnw723JMKtEWekFSYrRZXFi4Of8cPO8oXn/Bb7dP+MCEgXDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a240f04b6a86d0d770a02a68c3d6bcc1f5d62393bc253257fad4b9a9ba3cf5a","last_reissued_at":"2026-05-18T01:26:09.480779Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:09.480779Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.08113","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":"2026-05-18T01:26:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iJrVIFbiAp3Dkn9CNoAEsnP6fmj5sAzJEfrFrBxSYOBN3vSKIkzt/tQH2myZqIzo2CvbonDtAtALLe8naOFQDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:55:59.795301Z"},"content_sha256":"5ebd03760ad152a52de1e70bf2e2eaec751d293576ea67fdbe0e88d9563f6174","schema_version":"1.0","event_id":"sha256:5ebd03760ad152a52de1e70bf2e2eaec751d293576ea67fdbe0e88d9563f6174"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:PISA6BFWVBWQ25YKAKTIYPLLZQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analysis of Forward-Backward and Lepton Polarization Asymmetries in $B\\to K_{1}\\ell^{+}\\ell^{-}$ Decays in the Two-Higgs-doublet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ishtiaq Ahmed, M. Jamil Aslam, Naveed Ahmed","submitted_at":"2015-09-27T17:36:45Z","abstract_excerpt":"The exclusive semileptonic $B\\to K_{1}(1270) \\ell^{+}\\ell^{-}$ ($\\ell=\\mu , \\tau$) decays are analyzed in variants of two Higgs double models (THDMs). The mass eigenstates $K_{1}(1270)$ and $K_{1}(1400)$ are the mixture of two axial-vector SU(3) $^{1}{P}_{1}$ and $^{3}{P}_{1}$ states with the mixing angle $\\theta_{K}$. Making use of the form factors calculated in the Light Cone QCD approach and by taking the mixing angle $\\theta_{K}=-34^{\\circ}$, the impact of the parameters of the THDMs on different asymmetries in above mentioned semileptonic $B$ meson decays are studied. In this context the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08113","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":"2026-05-18T01:26:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8SvlCPPMoQk7FBI4MA5tBuddfzXVNdK6RD9x4zXfYteNWHrranZleWBKozHlp2lL5TRgnnA0luyJDjRWwKpsAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:55:59.795962Z"},"content_sha256":"c95580be1de104008784085cd78d7910c35c06f88168fb0c864ab6eac73d8929","schema_version":"1.0","event_id":"sha256:c95580be1de104008784085cd78d7910c35c06f88168fb0c864ab6eac73d8929"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/bundle.json","state_url":"https://pith.science/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/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":"2026-05-25T18:55:59Z","links":{"resolver":"https://pith.science/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ","bundle":"https://pith.science/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/bundle.json","state":"https://pith.science/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PISA6BFWVBWQ25YKAKTIYPLLZQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:PISA6BFWVBWQ25YKAKTIYPLLZQ","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":"e4c922eb0f8a406ad233a54f324e1e2acc07acf92736a47c85db244646d33ad9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-27T17:36:45Z","title_canon_sha256":"e9aab299e33a30b4a8e0aa9d9f5d193fcffa82cd119d9f228dd271bd1638bc25"},"schema_version":"1.0","source":{"id":"1509.08113","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08113","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08113v1","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08113","created_at":"2026-05-18T01:26:09Z"},{"alias_kind":"pith_short_12","alias_value":"PISA6BFWVBWQ","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_16","alias_value":"PISA6BFWVBWQ25YK","created_at":"2026-05-18T12:29:37Z"},{"alias_kind":"pith_short_8","alias_value":"PISA6BFW","created_at":"2026-05-18T12:29:37Z"}],"graph_snapshots":[{"event_id":"sha256:c95580be1de104008784085cd78d7910c35c06f88168fb0c864ab6eac73d8929","target":"graph","created_at":"2026-05-18T01:26:09Z","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":"The exclusive semileptonic $B\\to K_{1}(1270) \\ell^{+}\\ell^{-}$ ($\\ell=\\mu , \\tau$) decays are analyzed in variants of two Higgs double models (THDMs). The mass eigenstates $K_{1}(1270)$ and $K_{1}(1400)$ are the mixture of two axial-vector SU(3) $^{1}{P}_{1}$ and $^{3}{P}_{1}$ states with the mixing angle $\\theta_{K}$. Making use of the form factors calculated in the Light Cone QCD approach and by taking the mixing angle $\\theta_{K}=-34^{\\circ}$, the impact of the parameters of the THDMs on different asymmetries in above mentioned semileptonic $B$ meson decays are studied. In this context the ","authors_text":"Ishtiaq Ahmed, M. Jamil Aslam, Naveed Ahmed","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-27T17:36:45Z","title":"Analysis of Forward-Backward and Lepton Polarization Asymmetries in $B\\to K_{1}\\ell^{+}\\ell^{-}$ Decays in the Two-Higgs-doublet Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08113","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":"sha256:5ebd03760ad152a52de1e70bf2e2eaec751d293576ea67fdbe0e88d9563f6174","target":"record","created_at":"2026-05-18T01:26:09Z","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":"e4c922eb0f8a406ad233a54f324e1e2acc07acf92736a47c85db244646d33ad9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-27T17:36:45Z","title_canon_sha256":"e9aab299e33a30b4a8e0aa9d9f5d193fcffa82cd119d9f228dd271bd1638bc25"},"schema_version":"1.0","source":{"id":"1509.08113","kind":"arxiv","version":1}},"canonical_sha256":"7a240f04b6a86d0d770a02a68c3d6bcc1f5d62393bc253257fad4b9a9ba3cf5a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7a240f04b6a86d0d770a02a68c3d6bcc1f5d62393bc253257fad4b9a9ba3cf5a","first_computed_at":"2026-05-18T01:26:09.480779Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:26:09.480779Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sJRmMfD6zHoXjDZ/dw8Emf1Y0HjJV7xbT7vbl0bnw723JMKtEWekFSYrRZXFi4Of8cPO8oXn/Bb7dP+MCEgXDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:26:09.481416Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.08113","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5ebd03760ad152a52de1e70bf2e2eaec751d293576ea67fdbe0e88d9563f6174","sha256:c95580be1de104008784085cd78d7910c35c06f88168fb0c864ab6eac73d8929"],"state_sha256":"506e6f7a0d53cd24e49e617c978db2e0bed97c9971af45c43a29f7ca29c1a0d1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ln0UCofG3Eq8MdshQKbjFVE1wtPxlci+a8GUkuujIhf1N/8/smqRtMWsBL8u6LvJpRO9skoPD65JsrnwL4h9Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:55:59.803759Z","bundle_sha256":"9f104fdfa63d76ba80e8f402ce2e03368c8d847e49c08359d631481560dc862b"}}