{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:UVOZUIVOSZZGFVWIVMUPME76P3","short_pith_number":"pith:UVOZUIVO","schema_version":"1.0","canonical_sha256":"a55d9a22ae967262d6c8ab28f613fe7ee11819de405ea44f8b8d54c7ca7699f0","source":{"kind":"arxiv","id":"2302.03383","version":3},"attestation_state":"computed","paper":{"title":"Vector Meson Gravitational Form Factors and Generalized Parton Distributions at finite temperature within the soft-wall AdS/QCD Model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Minaya Allahverdiyeva, Shahin Mamedov","submitted_at":"2023-02-07T10:42:38Z","abstract_excerpt":"We investigate the vector meson's gravitational form factors (GFFs) and generalized parton distributions (GPDs) at finite temperatures within the soft-wall AdS/ QCD model. The plotted soft-wall GFFs graphs at zero temperature are close to the hard-wall results [1]. The dependence on temperature of the GFFs and GPDs is studied using the thermal dilaton approach in the soft-wall model. Plots of thermal GFFs show that they decrease in temperature increase. Also, the gravitational radius of $\\rho$ meson decreases in temperature growth and becomes zero around the critical temperature $T_c=0.2 {\\rm\\"},"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":"2302.03383","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-02-07T10:42:38Z","cross_cats_sorted":[],"title_canon_sha256":"fe32da3e0ba6da43cf61b5dae549969ee63d6aae08e01e7413869897de39b664","abstract_canon_sha256":"9e482146ccc738f5d4dc221e64c95f3b0103eba4653bfa7cf1b62178b4e9e202"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:26:45.574777Z","signature_b64":"1WncRu2tYTYQUElLHATKs7NkbHO8K6HVvE8zcO754xtqTeYiZ2ZcSmIHQ/K4Rgn7FFmcw9+ray0ytkMGCRh0Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a55d9a22ae967262d6c8ab28f613fe7ee11819de405ea44f8b8d54c7ca7699f0","last_reissued_at":"2026-07-05T06:26:45.574287Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:26:45.574287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vector Meson Gravitational Form Factors and Generalized Parton Distributions at finite temperature within the soft-wall AdS/QCD Model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Minaya Allahverdiyeva, Shahin Mamedov","submitted_at":"2023-02-07T10:42:38Z","abstract_excerpt":"We investigate the vector meson's gravitational form factors (GFFs) and generalized parton distributions (GPDs) at finite temperatures within the soft-wall AdS/ QCD model. The plotted soft-wall GFFs graphs at zero temperature are close to the hard-wall results [1]. The dependence on temperature of the GFFs and GPDs is studied using the thermal dilaton approach in the soft-wall model. Plots of thermal GFFs show that they decrease in temperature increase. Also, the gravitational radius of $\\rho$ meson decreases in temperature growth and becomes zero around the critical temperature $T_c=0.2 {\\rm\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.03383","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/2302.03383/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":"2302.03383","created_at":"2026-07-05T06:26:45.574350+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.03383v3","created_at":"2026-07-05T06:26:45.574350+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.03383","created_at":"2026-07-05T06:26:45.574350+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVOZUIVOSZZG","created_at":"2026-07-05T06:26:45.574350+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVOZUIVOSZZGFVWI","created_at":"2026-07-05T06:26:45.574350+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVOZUIVO","created_at":"2026-07-05T06:26:45.574350+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":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3","json":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3.json","graph_json":"https://pith.science/api/pith-number/UVOZUIVOSZZGFVWIVMUPME76P3/graph.json","events_json":"https://pith.science/api/pith-number/UVOZUIVOSZZGFVWIVMUPME76P3/events.json","paper":"https://pith.science/paper/UVOZUIVO"},"agent_actions":{"view_html":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3","download_json":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3.json","view_paper":"https://pith.science/paper/UVOZUIVO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.03383&json=true","fetch_graph":"https://pith.science/api/pith-number/UVOZUIVOSZZGFVWIVMUPME76P3/graph.json","fetch_events":"https://pith.science/api/pith-number/UVOZUIVOSZZGFVWIVMUPME76P3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3/action/storage_attestation","attest_author":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3/action/author_attestation","sign_citation":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3/action/citation_signature","submit_replication":"https://pith.science/pith/UVOZUIVOSZZGFVWIVMUPME76P3/action/replication_record"}},"created_at":"2026-07-05T06:26:45.574350+00:00","updated_at":"2026-07-05T06:26:45.574350+00:00"}