{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:LSEV7QSO2RPZJC6FB7XPQRNFH7","short_pith_number":"pith:LSEV7QSO","canonical_record":{"source":{"id":"2505.01202","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-02T11:45:11Z","cross_cats_sorted":[],"title_canon_sha256":"04951011976d131979b7581183770f043a46d11abacf7379fece6302901e6c64","abstract_canon_sha256":"2d00b381bcf9c3649e1b726799fcec2851230ddcdfd2eb4e49e0d4ff2ae87a17"},"schema_version":"1.0"},"canonical_sha256":"5c895fc24ed45f948bc50feef845a53fff1f8ea9427e6566954c6b122a7e086b","source":{"kind":"arxiv","id":"2505.01202","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.01202","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"arxiv_version","alias_value":"2505.01202v1","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.01202","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_12","alias_value":"LSEV7QSO2RPZ","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_16","alias_value":"LSEV7QSO2RPZJC6F","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_8","alias_value":"LSEV7QSO","created_at":"2026-07-05T10:57:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:LSEV7QSO2RPZJC6FB7XPQRNFH7","target":"record","payload":{"canonical_record":{"source":{"id":"2505.01202","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-02T11:45:11Z","cross_cats_sorted":[],"title_canon_sha256":"04951011976d131979b7581183770f043a46d11abacf7379fece6302901e6c64","abstract_canon_sha256":"2d00b381bcf9c3649e1b726799fcec2851230ddcdfd2eb4e49e0d4ff2ae87a17"},"schema_version":"1.0"},"canonical_sha256":"5c895fc24ed45f948bc50feef845a53fff1f8ea9427e6566954c6b122a7e086b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:57:47.558336Z","signature_b64":"MScFwPYFk5YsNiM6mQPfDb+DoC0CuQdEEz7VZM3ahvPy415wuAdnlijHRt636Swcn7sl2wvcdjZ+YYt+5MccAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c895fc24ed45f948bc50feef845a53fff1f8ea9427e6566954c6b122a7e086b","last_reissued_at":"2026-07-05T10:57:47.557807Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:57:47.557807Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2505.01202","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":"2026-07-05T10:57:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rVQGgeBOuxl550ntSDmgznzkta4JqD9s6MMNuAeXWC5aQt9i6JJn6l6xBqWKTQ8SLKtg4r4kAmLeILo1dfXMAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-17T09:31:06.859855Z"},"content_sha256":"303505c215dd405fbe13ed08c266758d38aa375f279cf6de814556a937f22469","schema_version":"1.0","event_id":"sha256:303505c215dd405fbe13ed08c266758d38aa375f279cf6de814556a937f22469"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:LSEV7QSO2RPZJC6FB7XPQRNFH7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Valence quark properties of charged kaons in symmetric nuclear matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arvind Kumar, Harleen Dahiya, Navpreet Kaur, Reetanshu Pandey, Satyajit Puhan, Suneel Dutt","submitted_at":"2025-05-02T11:45:11Z","abstract_excerpt":"We calculate the leading twist valence quark transverse momentum parton distribution functions (TMDs) and generalized parton distributions (GPDs) of the charged kaons in an isospin symmetric nuclear matter at zero temperature by employing the light-cone quark model. The medium modifications of the unpolarized TMDs and GPDs have been carried out by taking inputs from the chiral SU($3$) quark mean field model. The electromagnetic form factors (EMFFs) and charge radii have been calculated from the unpolarized GPDs for both the vacuum and in-medium cases. We have also calculated the variation of a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.01202","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.01202/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:57:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tSYFDPh7nArFcWoAsz6md0YlBqXLt6yq8L4imqJsj6x20m/t0EDxyEgIDXoMVaRHnLYE108OY2n4GkLaXrVTCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-17T09:31:06.860224Z"},"content_sha256":"5d83b0b32492b2a2284db85703c6adef85acdb48e2de6d8b16dd7c9cdb3ae580","schema_version":"1.0","event_id":"sha256:5d83b0b32492b2a2284db85703c6adef85acdb48e2de6d8b16dd7c9cdb3ae580"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/bundle.json","state_url":"https://pith.science/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/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":"2026-07-17T09:31:06Z","links":{"resolver":"https://pith.science/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7","bundle":"https://pith.science/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/bundle.json","state":"https://pith.science/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LSEV7QSO2RPZJC6FB7XPQRNFH7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:LSEV7QSO2RPZJC6FB7XPQRNFH7","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":"2d00b381bcf9c3649e1b726799fcec2851230ddcdfd2eb4e49e0d4ff2ae87a17","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-02T11:45:11Z","title_canon_sha256":"04951011976d131979b7581183770f043a46d11abacf7379fece6302901e6c64"},"schema_version":"1.0","source":{"id":"2505.01202","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.01202","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"arxiv_version","alias_value":"2505.01202v1","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.01202","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_12","alias_value":"LSEV7QSO2RPZ","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_16","alias_value":"LSEV7QSO2RPZJC6F","created_at":"2026-07-05T10:57:47Z"},{"alias_kind":"pith_short_8","alias_value":"LSEV7QSO","created_at":"2026-07-05T10:57:47Z"}],"graph_snapshots":[{"event_id":"sha256:5d83b0b32492b2a2284db85703c6adef85acdb48e2de6d8b16dd7c9cdb3ae580","target":"graph","created_at":"2026-07-05T10:57:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2505.01202/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the leading twist valence quark transverse momentum parton distribution functions (TMDs) and generalized parton distributions (GPDs) of the charged kaons in an isospin symmetric nuclear matter at zero temperature by employing the light-cone quark model. The medium modifications of the unpolarized TMDs and GPDs have been carried out by taking inputs from the chiral SU($3$) quark mean field model. The electromagnetic form factors (EMFFs) and charge radii have been calculated from the unpolarized GPDs for both the vacuum and in-medium cases. We have also calculated the variation of a","authors_text":"Arvind Kumar, Harleen Dahiya, Navpreet Kaur, Reetanshu Pandey, Satyajit Puhan, Suneel Dutt","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-02T11:45:11Z","title":"Valence quark properties of charged kaons in symmetric nuclear matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.01202","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":"sha256:303505c215dd405fbe13ed08c266758d38aa375f279cf6de814556a937f22469","target":"record","created_at":"2026-07-05T10:57:47Z","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":"2d00b381bcf9c3649e1b726799fcec2851230ddcdfd2eb4e49e0d4ff2ae87a17","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-02T11:45:11Z","title_canon_sha256":"04951011976d131979b7581183770f043a46d11abacf7379fece6302901e6c64"},"schema_version":"1.0","source":{"id":"2505.01202","kind":"arxiv","version":1}},"canonical_sha256":"5c895fc24ed45f948bc50feef845a53fff1f8ea9427e6566954c6b122a7e086b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c895fc24ed45f948bc50feef845a53fff1f8ea9427e6566954c6b122a7e086b","first_computed_at":"2026-07-05T10:57:47.557807Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:57:47.557807Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MScFwPYFk5YsNiM6mQPfDb+DoC0CuQdEEz7VZM3ahvPy415wuAdnlijHRt636Swcn7sl2wvcdjZ+YYt+5MccAA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:57:47.558336Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.01202","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:303505c215dd405fbe13ed08c266758d38aa375f279cf6de814556a937f22469","sha256:5d83b0b32492b2a2284db85703c6adef85acdb48e2de6d8b16dd7c9cdb3ae580"],"state_sha256":"7b10df63765f92b84b3b5a3fbe57972fb326c501c88b0091ba83dc7a6c14bf98"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GwvC/uaG3u2qLHqC5LxQv6VSCzzSRQGiEJ4DXsHE9oIAggwZ5NRSuyXw3cVwDHt5atkkfu2ZRYt3qWuxoGOwDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-17T09:31:06.862392Z","bundle_sha256":"08fec3427194e3b481da4fa41a068ca66f2c18e3fcd11f01f656b504f807f544"}}