{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:CSI66G2MO36FMGUSXGQUDJOEKP","short_pith_number":"pith:CSI66G2M","schema_version":"1.0","canonical_sha256":"1491ef1b4c76fc561a92b9a141a5c453f7b53ac27218934d83e45bb7cdef4394","source":{"kind":"arxiv","id":"2501.01755","version":3},"attestation_state":"computed","paper":{"title":"Confining potential in holographic bottom-up QCD from WKB","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfredo Vega, Miguel Angel Martin Contreras, Mitsutoshi Fujita","submitted_at":"2025-01-03T10:57:13Z","abstract_excerpt":"By using the \\emph{Rydberg--Klein--Rees} (RKR) formulas to solve the inverse Schr\\\"{o}dinger problem, we found a confining bottom-up potential from a given eigenvalue spectrum. To illustrate this methodology, we consider the vector meson spectrum derived in the D3/D7 system as input data to derive the corresponding bottom-up confining potential that resembles the geometric structure of the so-called hardwall model. We compute some properties for this new bottom-up model, including the thermal deconfinement phase transition, the $\\rho$ radial Regge trajectory, and the configurational entropy."},"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":"2501.01755","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-01-03T10:57:13Z","cross_cats_sorted":[],"title_canon_sha256":"1fab947d27da4222f2c0a5df5592d4f0ca394ad8bb4443807077ace8651fb902","abstract_canon_sha256":"0709f2cf7f28a2a28b7ba4f0bbc74b0339c20fdf837ba13c9a5a45ab02214d2d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T02:03:47.731512Z","signature_b64":"yIzHmN98pQOfbEZy+yHxr5sknDtsYdEEEpIs9b/wbduE84tpr7LStBOUuKSNKkuibG2MQnZRCqBKOF8M+BN8BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1491ef1b4c76fc561a92b9a141a5c453f7b53ac27218934d83e45bb7cdef4394","last_reissued_at":"2026-05-26T02:03:47.730538Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T02:03:47.730538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confining potential in holographic bottom-up QCD from WKB","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfredo Vega, Miguel Angel Martin Contreras, Mitsutoshi Fujita","submitted_at":"2025-01-03T10:57:13Z","abstract_excerpt":"By using the \\emph{Rydberg--Klein--Rees} (RKR) formulas to solve the inverse Schr\\\"{o}dinger problem, we found a confining bottom-up potential from a given eigenvalue spectrum. To illustrate this methodology, we consider the vector meson spectrum derived in the D3/D7 system as input data to derive the corresponding bottom-up confining potential that resembles the geometric structure of the so-called hardwall model. We compute some properties for this new bottom-up model, including the thermal deconfinement phase transition, the $\\rho$ radial Regge trajectory, and the configurational entropy."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.01755","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/2501.01755/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":"2501.01755","created_at":"2026-05-26T02:03:47.730669+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.01755v3","created_at":"2026-05-26T02:03:47.730669+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.01755","created_at":"2026-05-26T02:03:47.730669+00:00"},{"alias_kind":"pith_short_12","alias_value":"CSI66G2MO36F","created_at":"2026-05-26T02:03:47.730669+00:00"},{"alias_kind":"pith_short_16","alias_value":"CSI66G2MO36FMGUS","created_at":"2026-05-26T02:03:47.730669+00:00"},{"alias_kind":"pith_short_8","alias_value":"CSI66G2M","created_at":"2026-05-26T02:03:47.730669+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP","json":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP.json","graph_json":"https://pith.science/api/pith-number/CSI66G2MO36FMGUSXGQUDJOEKP/graph.json","events_json":"https://pith.science/api/pith-number/CSI66G2MO36FMGUSXGQUDJOEKP/events.json","paper":"https://pith.science/paper/CSI66G2M"},"agent_actions":{"view_html":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP","download_json":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP.json","view_paper":"https://pith.science/paper/CSI66G2M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.01755&json=true","fetch_graph":"https://pith.science/api/pith-number/CSI66G2MO36FMGUSXGQUDJOEKP/graph.json","fetch_events":"https://pith.science/api/pith-number/CSI66G2MO36FMGUSXGQUDJOEKP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP/action/storage_attestation","attest_author":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP/action/author_attestation","sign_citation":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP/action/citation_signature","submit_replication":"https://pith.science/pith/CSI66G2MO36FMGUSXGQUDJOEKP/action/replication_record"}},"created_at":"2026-05-26T02:03:47.730669+00:00","updated_at":"2026-05-26T02:03:47.730669+00:00"}