{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:N5TO3JMLUF6BDVAFCHDUYMY32T","short_pith_number":"pith:N5TO3JML","schema_version":"1.0","canonical_sha256":"6f66eda58ba17c11d40511c74c331bd4fba70185ac513729a70b5f9626509349","source":{"kind":"arxiv","id":"1207.2644","version":1},"attestation_state":"computed","paper":{"title":"Soft wall model with inverse exponential profile as a model for the axial and pseudoscalar mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"S.S. Afonin","submitted_at":"2012-07-11T14:04:09Z","abstract_excerpt":"According to the conjecture of the gauge/gravity duality a strongly coupled 4D field theory may be described by a dual 5D theory which is a free field theory in the first approximation. The usual description of the axial-vector sector in the bottom-up AdS/QCD models includes, however, the quartic interaction with a bulk scalar field. The question appears whether it is possible to describe some aspects of the chiral symmetry breaking in a way more consistent with the original proposal, i.e. within a free 5D theory? We suggest that a natural candidate for this purpose is the soft-wall model with"},"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":"1207.2644","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-11T14:04:09Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ae4723efa435d867a4d04b554d081cef3abf7eeeeb84f778c98b80cb98a78842","abstract_canon_sha256":"492e66a78d3d688cfadfa4deb5730d261c6ec4fd46fd6b0ae3382a4a4cd1dd9d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:10.478794Z","signature_b64":"Qp/Ippfb7BE2ngXzsLhQkm9wBbe0iXnhS6+yP+Ft0xU6OqcVEB6Ma+YQpW9j/Is6FoYWtDHlTxpIY10wuTyQDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f66eda58ba17c11d40511c74c331bd4fba70185ac513729a70b5f9626509349","last_reissued_at":"2026-05-18T03:41:10.478185Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:10.478185Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Soft wall model with inverse exponential profile as a model for the axial and pseudoscalar mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"S.S. Afonin","submitted_at":"2012-07-11T14:04:09Z","abstract_excerpt":"According to the conjecture of the gauge/gravity duality a strongly coupled 4D field theory may be described by a dual 5D theory which is a free field theory in the first approximation. The usual description of the axial-vector sector in the bottom-up AdS/QCD models includes, however, the quartic interaction with a bulk scalar field. The question appears whether it is possible to describe some aspects of the chiral symmetry breaking in a way more consistent with the original proposal, i.e. within a free 5D theory? We suggest that a natural candidate for this purpose is the soft-wall model with"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.2644","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1207.2644","created_at":"2026-05-18T03:41:10.478267+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.2644v1","created_at":"2026-05-18T03:41:10.478267+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.2644","created_at":"2026-05-18T03:41:10.478267+00:00"},{"alias_kind":"pith_short_12","alias_value":"N5TO3JMLUF6B","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"N5TO3JMLUF6BDVAF","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"N5TO3JML","created_at":"2026-05-18T12:27:16.716162+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/N5TO3JMLUF6BDVAFCHDUYMY32T","json":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T.json","graph_json":"https://pith.science/api/pith-number/N5TO3JMLUF6BDVAFCHDUYMY32T/graph.json","events_json":"https://pith.science/api/pith-number/N5TO3JMLUF6BDVAFCHDUYMY32T/events.json","paper":"https://pith.science/paper/N5TO3JML"},"agent_actions":{"view_html":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T","download_json":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T.json","view_paper":"https://pith.science/paper/N5TO3JML","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.2644&json=true","fetch_graph":"https://pith.science/api/pith-number/N5TO3JMLUF6BDVAFCHDUYMY32T/graph.json","fetch_events":"https://pith.science/api/pith-number/N5TO3JMLUF6BDVAFCHDUYMY32T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T/action/storage_attestation","attest_author":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T/action/author_attestation","sign_citation":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T/action/citation_signature","submit_replication":"https://pith.science/pith/N5TO3JMLUF6BDVAFCHDUYMY32T/action/replication_record"}},"created_at":"2026-05-18T03:41:10.478267+00:00","updated_at":"2026-05-18T03:41:10.478267+00:00"}