{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:PGSNKTQEZLWUJ2L6MKWU4ECMTD","short_pith_number":"pith:PGSNKTQE","canonical_record":{"source":{"id":"1802.07711","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-02-21T18:34:27Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"50b1a221d67f4c14604db7f949a3efcd1efebd799e77c2a6b3cae395009fbeb7","abstract_canon_sha256":"42643c58cc05558c4a0299dc9a9c6ad834e7b3173e0167cc5284f0580821c9fc"},"schema_version":"1.0"},"canonical_sha256":"79a4d54e04caed44e97e62ad4e104c98fbed923bf2c2099a1b078309c099afe4","source":{"kind":"arxiv","id":"1802.07711","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.07711","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"arxiv_version","alias_value":"1802.07711v1","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.07711","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"pith_short_12","alias_value":"PGSNKTQEZLWU","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PGSNKTQEZLWUJ2L6","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PGSNKTQE","created_at":"2026-05-18T12:32:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:PGSNKTQEZLWUJ2L6MKWU4ECMTD","target":"record","payload":{"canonical_record":{"source":{"id":"1802.07711","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-02-21T18:34:27Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"50b1a221d67f4c14604db7f949a3efcd1efebd799e77c2a6b3cae395009fbeb7","abstract_canon_sha256":"42643c58cc05558c4a0299dc9a9c6ad834e7b3173e0167cc5284f0580821c9fc"},"schema_version":"1.0"},"canonical_sha256":"79a4d54e04caed44e97e62ad4e104c98fbed923bf2c2099a1b078309c099afe4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:08.300068Z","signature_b64":"hu5vc1Nb1mG5ZOL9L4IEl2wgpAujZYPTASlX4eC13RtiZgVkT/WGya2XD9d62WClo8Bqj2OC6DwwnftvowSSBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"79a4d54e04caed44e97e62ad4e104c98fbed923bf2c2099a1b078309c099afe4","last_reissued_at":"2026-05-18T00:19:08.299328Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:08.299328Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1802.07711","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":"2026-05-18T00:19:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8+OXec+uyYfYK6Cq5EYRt/j6GrKXuSG7H5etn9az/e4rTY1TYYh06pKXcvykOICgqZK+dJUxuVQFOSd2k0PRCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T08:39:08.859154Z"},"content_sha256":"f6910977b7307da7989415e7cc7c4fba91a5203a76f8c36306aa993277bca5a5","schema_version":"1.0","event_id":"sha256:f6910977b7307da7989415e7cc7c4fba91a5203a76f8c36306aa993277bca5a5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:PGSNKTQEZLWUJ2L6MKWU4ECMTD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The electromagnetic multipole moments of the charged open-flavor $Z_{\\bar cq}$ states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"K. Azizi, U. Ozdem","submitted_at":"2018-02-21T18:34:27Z","abstract_excerpt":"The electromagnetic multipole moments of the open-flavor $Z_{\\bar cq}$ states are investigated by assuming a diquark-antidiquark picture for their internal structure and quantum numbers $J^{PC} = 1^{+-}$ for their spin-parity. In particular, their magnetic and quadrupole moments are extracted in the framework of light-cone QCD sum rule by the help of the photon distribution amplitudes. The electromagnetic multipole moments of the open-flavor $Z_{\\bar cq}$ states are important dynamical observables, which encode valuable information on their underlying structure. The results obtained for the ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.07711","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":"2026-05-18T00:19:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sxXPF7eAppgZH8r0jcAe0I58DBNwYq7iYPQLlfXfQn0X+lkJVrPt/oG9seNdgAy0N6DuPfeWdTlsPfOKoOUHCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T08:39:08.859511Z"},"content_sha256":"dc784b0cee8a8f0f2ee1f7980c49312c4859f3f94324e65581f7a2e76d3c2165","schema_version":"1.0","event_id":"sha256:dc784b0cee8a8f0f2ee1f7980c49312c4859f3f94324e65581f7a2e76d3c2165"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/bundle.json","state_url":"https://pith.science/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/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":"2026-06-02T08:39:08Z","links":{"resolver":"https://pith.science/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD","bundle":"https://pith.science/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/bundle.json","state":"https://pith.science/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PGSNKTQEZLWUJ2L6MKWU4ECMTD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:PGSNKTQEZLWUJ2L6MKWU4ECMTD","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":"42643c58cc05558c4a0299dc9a9c6ad834e7b3173e0167cc5284f0580821c9fc","cross_cats_sorted":["hep-ex","hep-lat"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-02-21T18:34:27Z","title_canon_sha256":"50b1a221d67f4c14604db7f949a3efcd1efebd799e77c2a6b3cae395009fbeb7"},"schema_version":"1.0","source":{"id":"1802.07711","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.07711","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"arxiv_version","alias_value":"1802.07711v1","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.07711","created_at":"2026-05-18T00:19:08Z"},{"alias_kind":"pith_short_12","alias_value":"PGSNKTQEZLWU","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PGSNKTQEZLWUJ2L6","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PGSNKTQE","created_at":"2026-05-18T12:32:43Z"}],"graph_snapshots":[{"event_id":"sha256:dc784b0cee8a8f0f2ee1f7980c49312c4859f3f94324e65581f7a2e76d3c2165","target":"graph","created_at":"2026-05-18T00:19:08Z","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 electromagnetic multipole moments of the open-flavor $Z_{\\bar cq}$ states are investigated by assuming a diquark-antidiquark picture for their internal structure and quantum numbers $J^{PC} = 1^{+-}$ for their spin-parity. In particular, their magnetic and quadrupole moments are extracted in the framework of light-cone QCD sum rule by the help of the photon distribution amplitudes. The electromagnetic multipole moments of the open-flavor $Z_{\\bar cq}$ states are important dynamical observables, which encode valuable information on their underlying structure. The results obtained for the ma","authors_text":"K. Azizi, U. Ozdem","cross_cats":["hep-ex","hep-lat"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-02-21T18:34:27Z","title":"The electromagnetic multipole moments of the charged open-flavor $Z_{\\bar cq}$ states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.07711","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:f6910977b7307da7989415e7cc7c4fba91a5203a76f8c36306aa993277bca5a5","target":"record","created_at":"2026-05-18T00:19:08Z","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":"42643c58cc05558c4a0299dc9a9c6ad834e7b3173e0167cc5284f0580821c9fc","cross_cats_sorted":["hep-ex","hep-lat"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-02-21T18:34:27Z","title_canon_sha256":"50b1a221d67f4c14604db7f949a3efcd1efebd799e77c2a6b3cae395009fbeb7"},"schema_version":"1.0","source":{"id":"1802.07711","kind":"arxiv","version":1}},"canonical_sha256":"79a4d54e04caed44e97e62ad4e104c98fbed923bf2c2099a1b078309c099afe4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"79a4d54e04caed44e97e62ad4e104c98fbed923bf2c2099a1b078309c099afe4","first_computed_at":"2026-05-18T00:19:08.299328Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:19:08.299328Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hu5vc1Nb1mG5ZOL9L4IEl2wgpAujZYPTASlX4eC13RtiZgVkT/WGya2XD9d62WClo8Bqj2OC6DwwnftvowSSBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:19:08.300068Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.07711","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f6910977b7307da7989415e7cc7c4fba91a5203a76f8c36306aa993277bca5a5","sha256:dc784b0cee8a8f0f2ee1f7980c49312c4859f3f94324e65581f7a2e76d3c2165"],"state_sha256":"751223aa19afea266ef12aefae12019019e8d91c59916b8518427e46ab5e8682"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ne87aoaacVgUqMKDAeQ+0msw+frlDD0JXaWThbm4naBulVsZvp+3X16gmCZYpwdJ0Geg7LRAEJ/aFdyWd97fBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T08:39:08.861447Z","bundle_sha256":"b1fcaedebcd6cf310a0090b2cf6d6ce0d3c4d6ba5b2e60f9747132274b9113b0"}}