{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:EUOGZG5PUTATINN3WZFQKBAAML","short_pith_number":"pith:EUOGZG5P","canonical_record":{"source":{"id":"2607.27653","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-30T04:06:09Z","cross_cats_sorted":["hep-ex","hep-lat","hep-th"],"title_canon_sha256":"1e81d60009c6385eb564e63d6ecdc94d94836ade51f78560985600af7d1b212c","abstract_canon_sha256":"718e3cfadabee89e75bd9a474cbbc666e7cec8206032a538b3b64722ac3d064e"},"schema_version":"1.0"},"canonical_sha256":"251c6c9bafa4c13435bbb64b05040062ff296e2d0f6e7e65d1b645fc8c7ad5ab","source":{"kind":"arxiv","id":"2607.27653","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.27653","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"arxiv_version","alias_value":"2607.27653v1","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.27653","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_12","alias_value":"EUOGZG5PUTAT","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"EUOGZG5PUTATINN3","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"EUOGZG5P","created_at":"2026-07-31T01:29:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:EUOGZG5PUTATINN3WZFQKBAAML","target":"record","payload":{"canonical_record":{"source":{"id":"2607.27653","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-30T04:06:09Z","cross_cats_sorted":["hep-ex","hep-lat","hep-th"],"title_canon_sha256":"1e81d60009c6385eb564e63d6ecdc94d94836ade51f78560985600af7d1b212c","abstract_canon_sha256":"718e3cfadabee89e75bd9a474cbbc666e7cec8206032a538b3b64722ac3d064e"},"schema_version":"1.0"},"canonical_sha256":"251c6c9bafa4c13435bbb64b05040062ff296e2d0f6e7e65d1b645fc8c7ad5ab","receipt":{"kind":"pith_receipt","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"251c6c9bafa4c13435bbb64b05040062ff296e2d0f6e7e65d1b645fc8c7ad5ab","last_reissued_at":"2026-07-31T01:29:22.394706Z","signature_status":"unsigned_v0","first_computed_at":"2026-07-31T01:29:22.394706Z"},"source_kind":"arxiv","source_id":"2607.27653","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":"2026-07-31T01:29:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tEgB+JuTn7DVhfTwBXqdOa4wsRyZM74BoxrjHCqTQ9ULkLK7vHoPVS31F1xHIlQvrQkCvXlh/tfYp7Sn65/GCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:49:24.809079Z"},"content_sha256":"abe3d017042cbb2978ea1bfa94eebdd04d797c9738f9fd55c32756b15cedc714","schema_version":"1.0","event_id":"sha256:abe3d017042cbb2978ea1bfa94eebdd04d797c9738f9fd55c32756b15cedc714"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:EUOGZG5PUTATINN3WZFQKBAAML","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetic dipole moments as probes of doubly-bottom molecular pentaquarks","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Ula\\c{s} \\\"{O}zdem","submitted_at":"2026-07-30T04:06:09Z","abstract_excerpt":"We investigate the magnetic dipole moments of doubly-bottom pentaquark states with spin-parities $J^P=\\tfrac{1}{2}^-$ and $\\tfrac{3}{2}^-$, interpreted as hadronic molecules in the $B\\Sigma_b$, $B\\Sigma_b^{*}$, and $B^{*}\\Sigma_b$ configurations. The analysis is performed within the framework of QCD light-cone sum rules employing photon distribution amplitudes. Our results demonstrate a strong sensitivity of the magnetic dipole moments to the internal spin structure and quark composition of the states. In particular, the light-quark sector provides the dominant contribution in the $B\\Sigma_b$ "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.27653","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.27653/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-31T01:29:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K10UIUrLy0iU3TFBpdzdVN3pjfNugN4t6XYdnJd/2HKWvqNoHG1hNmb45SXmL07pphiao6I1FS477Xs8xAyHAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:49:24.809568Z"},"content_sha256":"e33393858179e8088660ab1e18b13b3d6b4e77cc34bf3ab51b818e33f9bd6c1c","schema_version":"1.0","event_id":"sha256:e33393858179e8088660ab1e18b13b3d6b4e77cc34bf3ab51b818e33f9bd6c1c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EUOGZG5PUTATINN3WZFQKBAAML/bundle.json","state_url":"https://pith.science/pith/EUOGZG5PUTATINN3WZFQKBAAML/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EUOGZG5PUTATINN3WZFQKBAAML/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":"2026-08-03T22:49:24Z","links":{"resolver":"https://pith.science/pith/EUOGZG5PUTATINN3WZFQKBAAML","bundle":"https://pith.science/pith/EUOGZG5PUTATINN3WZFQKBAAML/bundle.json","state":"https://pith.science/pith/EUOGZG5PUTATINN3WZFQKBAAML/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EUOGZG5PUTATINN3WZFQKBAAML/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:EUOGZG5PUTATINN3WZFQKBAAML","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":"718e3cfadabee89e75bd9a474cbbc666e7cec8206032a538b3b64722ac3d064e","cross_cats_sorted":["hep-ex","hep-lat","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-30T04:06:09Z","title_canon_sha256":"1e81d60009c6385eb564e63d6ecdc94d94836ade51f78560985600af7d1b212c"},"schema_version":"1.0","source":{"id":"2607.27653","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.27653","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"arxiv_version","alias_value":"2607.27653v1","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.27653","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_12","alias_value":"EUOGZG5PUTAT","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"EUOGZG5PUTATINN3","created_at":"2026-07-31T01:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"EUOGZG5P","created_at":"2026-07-31T01:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:e33393858179e8088660ab1e18b13b3d6b4e77cc34bf3ab51b818e33f9bd6c1c","target":"graph","created_at":"2026-07-31T01:29:22Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2607.27653/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the magnetic dipole moments of doubly-bottom pentaquark states with spin-parities $J^P=\\tfrac{1}{2}^-$ and $\\tfrac{3}{2}^-$, interpreted as hadronic molecules in the $B\\Sigma_b$, $B\\Sigma_b^{*}$, and $B^{*}\\Sigma_b$ configurations. The analysis is performed within the framework of QCD light-cone sum rules employing photon distribution amplitudes. Our results demonstrate a strong sensitivity of the magnetic dipole moments to the internal spin structure and quark composition of the states. In particular, the light-quark sector provides the dominant contribution in the $B\\Sigma_b$ ","authors_text":"Ula\\c{s} \\\"{O}zdem","cross_cats":["hep-ex","hep-lat","hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-30T04:06:09Z","title":"Magnetic dipole moments as probes of doubly-bottom molecular pentaquarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.27653","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:abe3d017042cbb2978ea1bfa94eebdd04d797c9738f9fd55c32756b15cedc714","target":"record","created_at":"2026-07-31T01:29:22Z","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":"718e3cfadabee89e75bd9a474cbbc666e7cec8206032a538b3b64722ac3d064e","cross_cats_sorted":["hep-ex","hep-lat","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-30T04:06:09Z","title_canon_sha256":"1e81d60009c6385eb564e63d6ecdc94d94836ade51f78560985600af7d1b212c"},"schema_version":"1.0","source":{"id":"2607.27653","kind":"arxiv","version":1}},"canonical_sha256":"251c6c9bafa4c13435bbb64b05040062ff296e2d0f6e7e65d1b645fc8c7ad5ab","receipt":{"builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"251c6c9bafa4c13435bbb64b05040062ff296e2d0f6e7e65d1b645fc8c7ad5ab","first_computed_at":"2026-07-31T01:29:22.394706Z","kind":"pith_receipt","last_reissued_at":"2026-07-31T01:29:22.394706Z","receipt_version":"0.3","signature_status":"unsigned_v0"},"source_id":"2607.27653","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:abe3d017042cbb2978ea1bfa94eebdd04d797c9738f9fd55c32756b15cedc714","sha256:e33393858179e8088660ab1e18b13b3d6b4e77cc34bf3ab51b818e33f9bd6c1c"],"state_sha256":"b76309b17cdd4e6b96b9b77333db8c460bb3ec670ee36c82f59f03b07ad92f12"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GtD6NCzkF9sZ2mDe+aN1d3sY3L9B8DGQpyiLrwCO9PCfWXX7Zp3kheTVomV5kQ77cFetdDT8eFenhkrDUUcCDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T22:49:24.814943Z","bundle_sha256":"c042dfd45be07cfaf138082ff9545110c8734ddcadcb3cae47de6597daa5ed4c"}}