{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:UAWX7UWNL4KIKDFIOPY7HOYW7T","short_pith_number":"pith:UAWX7UWN","schema_version":"1.0","canonical_sha256":"a02d7fd2cd5f14850ca873f1f3bb16fce50e3e7113aea6ffe921c660e8f9d52b","source":{"kind":"arxiv","id":"2204.06205","version":3},"attestation_state":"computed","paper":{"title":"Deuteron electromagnetic form factors and tensor polarization observables in the framework of the hard-wall AdS/QCD model","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Jannat Samadov, Narmin Huseynova, Shahin Mamedov","submitted_at":"2022-04-13T07:20:54Z","abstract_excerpt":"We study the electromagnetic form factors and tensor polarization observables of the deuteron in the framework of the hard-wall AdS/QCD model. We find a profile function for the bulk twist $\\tau=6$ vector field, which describes the deuteron on the boundary and fix the infrared boundary cut-off of AdS space in accordance with the ground state mass of the deuteron. We obtain the deuteron charge monopole, quadrupole, and magnetic dipole form factors and tensor polarization observables from the bulk Lagrangians for the deuteron and photon field interactions. We plot the momentum transfer dependenc"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2204.06205","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"hep-ph","submitted_at":"2022-04-13T07:20:54Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"2668cd35415ef53eac14f97320c590f0ff06a8fc9b5e14b16361062c875ad51a","abstract_canon_sha256":"590c8d59b88b41bc63ba0ecdcb945adc766e7282de4efc7ad718c37d544722bd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:42:00.825341Z","signature_b64":"U3xrhxjreETT64ijCgyKQEXXDtfHay8U7X03jpD7vnmlWijWzbWkRIcWE6IbUbZBZtW+knY5wCdBUuTcHquMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a02d7fd2cd5f14850ca873f1f3bb16fce50e3e7113aea6ffe921c660e8f9d52b","last_reissued_at":"2026-07-05T05:42:00.824913Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:42:00.824913Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deuteron electromagnetic form factors and tensor polarization observables in the framework of the hard-wall AdS/QCD model","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Jannat Samadov, Narmin Huseynova, Shahin Mamedov","submitted_at":"2022-04-13T07:20:54Z","abstract_excerpt":"We study the electromagnetic form factors and tensor polarization observables of the deuteron in the framework of the hard-wall AdS/QCD model. We find a profile function for the bulk twist $\\tau=6$ vector field, which describes the deuteron on the boundary and fix the infrared boundary cut-off of AdS space in accordance with the ground state mass of the deuteron. We obtain the deuteron charge monopole, quadrupole, and magnetic dipole form factors and tensor polarization observables from the bulk Lagrangians for the deuteron and photon field interactions. We plot the momentum transfer dependenc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.06205","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2204.06205/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2204.06205","created_at":"2026-07-05T05:42:00.824968+00:00"},{"alias_kind":"arxiv_version","alias_value":"2204.06205v3","created_at":"2026-07-05T05:42:00.824968+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.06205","created_at":"2026-07-05T05:42:00.824968+00:00"},{"alias_kind":"pith_short_12","alias_value":"UAWX7UWNL4KI","created_at":"2026-07-05T05:42:00.824968+00:00"},{"alias_kind":"pith_short_16","alias_value":"UAWX7UWNL4KIKDFI","created_at":"2026-07-05T05:42:00.824968+00:00"},{"alias_kind":"pith_short_8","alias_value":"UAWX7UWN","created_at":"2026-07-05T05:42:00.824968+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21706","citing_title":"Generalized parton distributions of a deuteron in an AdS/QCD hard-wall model","ref_index":33,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T","json":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T.json","graph_json":"https://pith.science/api/pith-number/UAWX7UWNL4KIKDFIOPY7HOYW7T/graph.json","events_json":"https://pith.science/api/pith-number/UAWX7UWNL4KIKDFIOPY7HOYW7T/events.json","paper":"https://pith.science/paper/UAWX7UWN"},"agent_actions":{"view_html":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T","download_json":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T.json","view_paper":"https://pith.science/paper/UAWX7UWN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2204.06205&json=true","fetch_graph":"https://pith.science/api/pith-number/UAWX7UWNL4KIKDFIOPY7HOYW7T/graph.json","fetch_events":"https://pith.science/api/pith-number/UAWX7UWNL4KIKDFIOPY7HOYW7T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T/action/storage_attestation","attest_author":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T/action/author_attestation","sign_citation":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T/action/citation_signature","submit_replication":"https://pith.science/pith/UAWX7UWNL4KIKDFIOPY7HOYW7T/action/replication_record"}},"created_at":"2026-07-05T05:42:00.824968+00:00","updated_at":"2026-07-05T05:42:00.824968+00:00"}