{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:7QLCSMJ3FVSQGKQVUFU5IG43DG","short_pith_number":"pith:7QLCSMJ3","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"},"canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","source":{"kind":"arxiv","id":"1706.08895","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.08895","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"arxiv_version","alias_value":"1706.08895v1","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.08895","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"pith_short_12","alias_value":"7QLCSMJ3FVSQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"7QLCSMJ3FVSQGKQV","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"7QLCSMJ3","created_at":"2026-05-18T12:31:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:7QLCSMJ3FVSQGKQVUFU5IG43DG","target":"record","payload":{"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"},"canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","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"},"source_kind":"arxiv","source_id":"1706.08895","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:10:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hA5zc0dqJjFCj47PRxsyESv9YKPpWYvA7U6Lr90ydo9dRS8WwO9T24qIlNHMjohkI2ovyOJ4qFLcR2ROod0WCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T21:34:51.268719Z"},"content_sha256":"a8d92b8181a4a077aa1532f9b0c6a5b54e6f8786efb35125ec63db40a0e57037","schema_version":"1.0","event_id":"sha256:a8d92b8181a4a077aa1532f9b0c6a5b54e6f8786efb35125ec63db40a0e57037"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:7QLCSMJ3FVSQGKQVUFU5IG43DG","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:10:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"We++TNrLp+2ii06CD/GmMi66brQLnzh4jENje/uv9C6j9+EOGiMe9mLLN6j5LIQoMJG0lJRpcwbGBANqbHhOCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T21:34:51.269387Z"},"content_sha256":"640f2a32ca95f2845abf2524a7d6b75e5cd99bd58418e641d115d08739b3cdf3","schema_version":"1.0","event_id":"sha256:640f2a32ca95f2845abf2524a7d6b75e5cd99bd58418e641d115d08739b3cdf3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/bundle.json","state_url":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-29T21:34:51Z","links":{"resolver":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG","bundle":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/bundle.json","state":"https://pith.science/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7QLCSMJ3FVSQGKQVUFU5IG43DG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:7QLCSMJ3FVSQGKQVUFU5IG43DG","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"02cb73bb2823d8476b424c6b965881a25b6ebaff242a2e56eed3503b4f2802cd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-27T14:51:17Z","title_canon_sha256":"33a73487660f7e717f80fa926692057103e1745e0d4cf5ecb8473e055bdbb19b"},"schema_version":"1.0","source":{"id":"1706.08895","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.08895","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"arxiv_version","alias_value":"1706.08895v1","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.08895","created_at":"2026-05-18T00:10:24Z"},{"alias_kind":"pith_short_12","alias_value":"7QLCSMJ3FVSQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"7QLCSMJ3FVSQGKQV","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"7QLCSMJ3","created_at":"2026-05-18T12:31:05Z"}],"graph_snapshots":[{"event_id":"sha256:640f2a32ca95f2845abf2524a7d6b75e5cd99bd58418e641d115d08739b3cdf3","target":"graph","created_at":"2026-05-18T00:10:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"Arghya Mukherjee, Mahatsab Mandal, Pradip Roy, Snigdha Ghosh, Sourav Sarkar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-27T14:51:17Z","title":"$\\rho^0-\\omega$ mixing in the presence of a weak magnetic field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.08895","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a8d92b8181a4a077aa1532f9b0c6a5b54e6f8786efb35125ec63db40a0e57037","target":"record","created_at":"2026-05-18T00:10:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"02cb73bb2823d8476b424c6b965881a25b6ebaff242a2e56eed3503b4f2802cd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-27T14:51:17Z","title_canon_sha256":"33a73487660f7e717f80fa926692057103e1745e0d4cf5ecb8473e055bdbb19b"},"schema_version":"1.0","source":{"id":"1706.08895","kind":"arxiv","version":1}},"canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fc1629313b2d65032a15a169d41b9b1989cd6b43c6b8073422a9dedc862c9dc4","first_computed_at":"2026-05-18T00:10:24.448993Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:10:24.448993Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xyNX3mf2o6ZX8xRuBkLwNDBYnj5JmeaoEpORjI+ac7eBrDCh7wF5fD2+Le7fhlsWthomU4O+bujklLqt4LpKCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:10:24.449592Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.08895","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a8d92b8181a4a077aa1532f9b0c6a5b54e6f8786efb35125ec63db40a0e57037","sha256:640f2a32ca95f2845abf2524a7d6b75e5cd99bd58418e641d115d08739b3cdf3"],"state_sha256":"d184dc26e7d276176def2c10a35f16ab103bdf6704362159002030198c75d3fe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4yYfq+SWIW+FU5XJM63no+j2cGoh5qYW6EFxrgO/eZH+AG6Z/QQ/TUFYWDx7p1qHPTmpdaSlRwoRoh4DjAk5BA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T21:34:51.272865Z","bundle_sha256":"f5d56d41eb2e33bb6fbf3a26ec237f9c522ec638063268ec420929a965538ea7"}}