{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:JHYLZP467L6NGAGKWAE7MIJHQ5","short_pith_number":"pith:JHYLZP46","canonical_record":{"source":{"id":"1903.07340","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-03-18T10:01:32Z","cross_cats_sorted":[],"title_canon_sha256":"0ec99064a52b0d733d1d182d65746ab2ed87fea4cfeff4b66108a827144e9c19","abstract_canon_sha256":"3ce8a10c21e32b8f2344ba44609ee8d87555a7f7cf818b603e1ef93a16373314"},"schema_version":"1.0"},"canonical_sha256":"49f0bcbf9efafcd300cab009f62127875ede0f9edd78416521e2e6948acc1ec5","source":{"kind":"arxiv","id":"1903.07340","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1903.07340","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"arxiv_version","alias_value":"1903.07340v1","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.07340","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"pith_short_12","alias_value":"JHYLZP467L6N","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_16","alias_value":"JHYLZP467L6NGAGK","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_8","alias_value":"JHYLZP46","created_at":"2026-05-18T12:33:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:JHYLZP467L6NGAGKWAE7MIJHQ5","target":"record","payload":{"canonical_record":{"source":{"id":"1903.07340","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-03-18T10:01:32Z","cross_cats_sorted":[],"title_canon_sha256":"0ec99064a52b0d733d1d182d65746ab2ed87fea4cfeff4b66108a827144e9c19","abstract_canon_sha256":"3ce8a10c21e32b8f2344ba44609ee8d87555a7f7cf818b603e1ef93a16373314"},"schema_version":"1.0"},"canonical_sha256":"49f0bcbf9efafcd300cab009f62127875ede0f9edd78416521e2e6948acc1ec5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:45.056723Z","signature_b64":"O1T6tFf6XM/mf/07hyo7yvR0x69+WGJ/LlHBRHJuAvooo67b1NUNtvdlgHAq/PuNdCFmkuVm8lLEE17BHtb8AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49f0bcbf9efafcd300cab009f62127875ede0f9edd78416521e2e6948acc1ec5","last_reissued_at":"2026-05-17T23:48:45.056068Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:45.056068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1903.07340","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":"2026-05-17T23:48:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9CmUKLs/pzCsIjNsQbdpxJ7NBP+MWBkezDkwXbeiwC3tinwoV6GhpkrJnXj4wItdquPP7ZncvJKinUiHkXXQDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T20:34:08.666609Z"},"content_sha256":"3e47c2b62d396dd3428ed1fcf5a7be09d5593a255307486ef1a4cd0cc9015f77","schema_version":"1.0","event_id":"sha256:3e47c2b62d396dd3428ed1fcf5a7be09d5593a255307486ef1a4cd0cc9015f77"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:JHYLZP467L6NGAGKWAE7MIJHQ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Structure, formation and decay of $\\bar{K}NN$ system by Faddeev-AGS calculations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Esmaili, Sajjad Marri, S. Z. Kalantari","submitted_at":"2019-03-18T10:01:32Z","abstract_excerpt":"The Faddeev AGS equations are solved for coupled-channels $\\bar{K}NN-\\pi\\Sigma{N}$ system with quantum numbers $I=1/2$ and $S=0$. Using separable potentials for $\\bar{K}N-\\pi\\Sigma$ interaction, we have calculated the transition probability for the $(Y_{K})_{I=0}+N\\rightarrow\\pi\\Sigma{N}$ reaction. The possibility to observe the trace of $K^{-}pp$ quasi-bound state in the $\\pi\\Sigma{N}$ mass spectra was studied. Various types of chiral based and phenomenological potentials are used to describe the $\\bar{K}N-\\pi\\Sigma$ interaction. It was shown that not only we can see the signature of the $K^{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.07340","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":"2026-05-17T23:48:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kmMO4HGo+B3EaHHTGlvaEnPztITcbtj6VWFsh7nMmfeX+RaoXKSSQJzsoZDmGQVE1GLN2F8fkJsHZ9RbQALRBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T20:34:08.667338Z"},"content_sha256":"db556942a2135b1d184f6f0e4c669fa3e59646ba5f66281c88706eedec54c9b0","schema_version":"1.0","event_id":"sha256:db556942a2135b1d184f6f0e4c669fa3e59646ba5f66281c88706eedec54c9b0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/bundle.json","state_url":"https://pith.science/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/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":"2026-06-05T20:34:08Z","links":{"resolver":"https://pith.science/pith/JHYLZP467L6NGAGKWAE7MIJHQ5","bundle":"https://pith.science/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/bundle.json","state":"https://pith.science/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JHYLZP467L6NGAGKWAE7MIJHQ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:JHYLZP467L6NGAGKWAE7MIJHQ5","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":"3ce8a10c21e32b8f2344ba44609ee8d87555a7f7cf818b603e1ef93a16373314","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-03-18T10:01:32Z","title_canon_sha256":"0ec99064a52b0d733d1d182d65746ab2ed87fea4cfeff4b66108a827144e9c19"},"schema_version":"1.0","source":{"id":"1903.07340","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1903.07340","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"arxiv_version","alias_value":"1903.07340v1","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.07340","created_at":"2026-05-17T23:48:45Z"},{"alias_kind":"pith_short_12","alias_value":"JHYLZP467L6N","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_16","alias_value":"JHYLZP467L6NGAGK","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_8","alias_value":"JHYLZP46","created_at":"2026-05-18T12:33:21Z"}],"graph_snapshots":[{"event_id":"sha256:db556942a2135b1d184f6f0e4c669fa3e59646ba5f66281c88706eedec54c9b0","target":"graph","created_at":"2026-05-17T23:48:45Z","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":"The Faddeev AGS equations are solved for coupled-channels $\\bar{K}NN-\\pi\\Sigma{N}$ system with quantum numbers $I=1/2$ and $S=0$. Using separable potentials for $\\bar{K}N-\\pi\\Sigma$ interaction, we have calculated the transition probability for the $(Y_{K})_{I=0}+N\\rightarrow\\pi\\Sigma{N}$ reaction. The possibility to observe the trace of $K^{-}pp$ quasi-bound state in the $\\pi\\Sigma{N}$ mass spectra was studied. Various types of chiral based and phenomenological potentials are used to describe the $\\bar{K}N-\\pi\\Sigma$ interaction. It was shown that not only we can see the signature of the $K^{","authors_text":"J. Esmaili, Sajjad Marri, S. Z. Kalantari","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-03-18T10:01:32Z","title":"Structure, formation and decay of $\\bar{K}NN$ system by Faddeev-AGS calculations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.07340","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":"sha256:3e47c2b62d396dd3428ed1fcf5a7be09d5593a255307486ef1a4cd0cc9015f77","target":"record","created_at":"2026-05-17T23:48:45Z","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":"3ce8a10c21e32b8f2344ba44609ee8d87555a7f7cf818b603e1ef93a16373314","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-03-18T10:01:32Z","title_canon_sha256":"0ec99064a52b0d733d1d182d65746ab2ed87fea4cfeff4b66108a827144e9c19"},"schema_version":"1.0","source":{"id":"1903.07340","kind":"arxiv","version":1}},"canonical_sha256":"49f0bcbf9efafcd300cab009f62127875ede0f9edd78416521e2e6948acc1ec5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"49f0bcbf9efafcd300cab009f62127875ede0f9edd78416521e2e6948acc1ec5","first_computed_at":"2026-05-17T23:48:45.056068Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:48:45.056068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O1T6tFf6XM/mf/07hyo7yvR0x69+WGJ/LlHBRHJuAvooo67b1NUNtvdlgHAq/PuNdCFmkuVm8lLEE17BHtb8AA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:48:45.056723Z","signed_message":"canonical_sha256_bytes"},"source_id":"1903.07340","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3e47c2b62d396dd3428ed1fcf5a7be09d5593a255307486ef1a4cd0cc9015f77","sha256:db556942a2135b1d184f6f0e4c669fa3e59646ba5f66281c88706eedec54c9b0"],"state_sha256":"1d988e90321d99fa15dcdb4cbc39945605ff211dc1e2a95b0df03d235e4f97ec"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hqGQ1DuRdUAI4G9tuFQ617E9acV1Oo1LzRobD80wP1LEGaYT68yHHNR9KTMBgSBWbo6C82MxU9/vJjYFDLcaAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T20:34:08.671390Z","bundle_sha256":"2effc7ad28ba38bfac6ed88b8bf30bb6e65facafd0003cfaee066b7800610e62"}}