{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:7QLCSMJ3FVSQGKQVUFU5IG43DG","short_pith_number":"pith:7QLCSMJ3","schema_version":"1.0","canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","source":{"kind":"arxiv","id":"1706.08895","version":1},"attestation_state":"computed","paper":{"title":"$\\rho^0-\\omega$ mixing in the presence of a weak magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arghya Mukherjee, Mahatsab Mandal, Pradip Roy, Snigdha Ghosh, Sourav Sarkar","submitted_at":"2017-06-27T14:51:17Z","abstract_excerpt":"We calculate the momentum dependence of the $\\rho^0-\\omega$ mixing amplitude in vacuum with vector nucleon-nucleon interaction in presence of a constant homogeneous weak magnetic field background. The mixing amplitude is generated by the nucleon-nucleon ($NN$) interaction and thus driven by the neutron-proton mass difference along with a constant magnetic field. We find a significant effect of magnetic field on the mixing amplitude. We also calculate the Charge symmetry violating (CSV) $NN$ potential induced by the magnetic field dependent mixing amplitude. The presence of the magnetic field i"},"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":"1706.08895","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-27T14:51:17Z","cross_cats_sorted":[],"title_canon_sha256":"33a73487660f7e717f80fa926692057103e1745e0d4cf5ecb8473e055bdbb19b","abstract_canon_sha256":"02cb73bb2823d8476b424c6b965881a25b6ebaff242a2e56eed3503b4f2802cd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:24.449592Z","signature_b64":"xyNX3mf2o6ZX8xRuBkLwNDBYnj5JmeaoEpORjI+ac7eBrDCh7wF5fD2+Le7fhlsWthomU4O+bujklLqt4LpKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","last_reissued_at":"2026-05-18T00:10:24.448993Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:24.448993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\rho^0-\\omega$ mixing in the presence of a weak magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arghya Mukherjee, Mahatsab Mandal, Pradip Roy, Snigdha Ghosh, Sourav Sarkar","submitted_at":"2017-06-27T14:51:17Z","abstract_excerpt":"We calculate the momentum dependence of the $\\rho^0-\\omega$ mixing amplitude in vacuum with vector nucleon-nucleon interaction in presence of a constant homogeneous weak magnetic field background. The mixing amplitude is generated by the nucleon-nucleon ($NN$) interaction and thus driven by the neutron-proton mass difference along with a constant magnetic field. We find a significant effect of magnetic field on the mixing amplitude. We also calculate the Charge symmetry violating (CSV) $NN$ potential induced by the magnetic field dependent mixing amplitude. The presence of the magnetic field i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.08895","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":"1706.08895","created_at":"2026-05-18T00:10:24.449105+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.08895v1","created_at":"2026-05-18T00:10:24.449105+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.08895","created_at":"2026-05-18T00:10:24.449105+00:00"},{"alias_kind":"pith_short_12","alias_value":"7QLCSMJ3FVSQ","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_16","alias_value":"7QLCSMJ3FVSQGKQV","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_8","alias_value":"7QLCSMJ3","created_at":"2026-05-18T12:31:05.417338+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/7QLCSMJ3FVSQGKQVUFU5IG43DG","json":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG.json","graph_json":"https://pith.science/api/pith-number/7QLCSMJ3FVSQGKQVUFU5IG43DG/graph.json","events_json":"https://pith.science/api/pith-number/7QLCSMJ3FVSQGKQVUFU5IG43DG/events.json","paper":"https://pith.science/paper/7QLCSMJ3"},"agent_actions":{"view_html":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG","download_json":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG.json","view_paper":"https://pith.science/paper/7QLCSMJ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.08895&json=true","fetch_graph":"https://pith.science/api/pith-number/7QLCSMJ3FVSQGKQVUFU5IG43DG/graph.json","fetch_events":"https://pith.science/api/pith-number/7QLCSMJ3FVSQGKQVUFU5IG43DG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/action/storage_attestation","attest_author":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/action/author_attestation","sign_citation":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/action/citation_signature","submit_replication":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/action/replication_record"}},"created_at":"2026-05-18T00:10:24.449105+00:00","updated_at":"2026-05-18T00:10:24.449105+00:00"}