{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:65LGXCU7ZK6MGDMUTC3OX3U3IY","short_pith_number":"pith:65LGXCU7","canonical_record":{"source":{"id":"1207.5279","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-07-23T02:23:37Z","cross_cats_sorted":[],"title_canon_sha256":"220b0ad080064dd56d1ae305e4d0ae52376f0595553394fa5f011e3aa4420863","abstract_canon_sha256":"90d4396f721099807f066910861910c3f875b8ddd22f13bfb5d5c2cfaa526610"},"schema_version":"1.0"},"canonical_sha256":"f7566b8a9fcabcc30d9498b6ebee9b460c1ff296ef42ab1239cbd5ab47525566","source":{"kind":"arxiv","id":"1207.5279","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5279","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5279v3","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5279","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"pith_short_12","alias_value":"65LGXCU7ZK6M","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"65LGXCU7ZK6MGDMU","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"65LGXCU7","created_at":"2026-05-18T12:26:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:65LGXCU7ZK6MGDMUTC3OX3U3IY","target":"record","payload":{"canonical_record":{"source":{"id":"1207.5279","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-07-23T02:23:37Z","cross_cats_sorted":[],"title_canon_sha256":"220b0ad080064dd56d1ae305e4d0ae52376f0595553394fa5f011e3aa4420863","abstract_canon_sha256":"90d4396f721099807f066910861910c3f875b8ddd22f13bfb5d5c2cfaa526610"},"schema_version":"1.0"},"canonical_sha256":"f7566b8a9fcabcc30d9498b6ebee9b460c1ff296ef42ab1239cbd5ab47525566","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:15.164269Z","signature_b64":"XmFihnch21E2jE5fk2SFl60fjpCGCixXmmq6MY0423ra1CDsvdCQU/bxh7gml9Bu7sRMnpT+y84GjmlD8vpCAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f7566b8a9fcabcc30d9498b6ebee9b460c1ff296ef42ab1239cbd5ab47525566","last_reissued_at":"2026-05-18T01:56:15.163679Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:15.163679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.5279","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:56:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nPiHg0WnR+99EpOc7SkJ+5aL4c9CobefkhqfvpDUocuMfPLB0rEfhje7xlZaTOpsIddRB2cgR+TD7YxX76KFCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:20:07.910491Z"},"content_sha256":"d470160dc76cf28ab58df64a99980a4fbed158dad64f552ed8b6b9b68d64f296","schema_version":"1.0","event_id":"sha256:d470160dc76cf28ab58df64a99980a4fbed158dad64f552ed8b6b9b68d64f296"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:65LGXCU7ZK6MGDMUTC3OX3U3IY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Comprehensive application of a coupled-channel complex scaling method to the KbarN-piY system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Akinobu Dote, Takashi Inoue, Takayuki Myo","submitted_at":"2012-07-23T02:23:37Z","abstract_excerpt":"We have applied the coupled-channel complex scaling method (ccCSM) to K^{bar}N-\\pi Y system. One advantage of ccCSM is that resonant states as well as scattering states can be treated in the same framework. For the interactions in the system, we have constructed a meson-baryon potential-matrix by basing on the chiral SU(3) theory and respecting the K^{bar}N scattering length obtained in the Martin's analysis. For future purpose to apply it more complicated system such as K^{bar}NN, we adopt a local Gaussian form in the r-space. We have investigated both the non-relativistic (NR) and the semi-r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5279","kind":"arxiv","version":3},"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":"2026-05-18T01:56:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"16wweSMCdEZPnrqFiWf7BufEV/ptKaVXfcTnrqU7cjMTixoz171v6bR55l7zfo843LWvVryjPgAC/gQyArJCAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:20:07.910838Z"},"content_sha256":"2bd1bc45c914d423fa8e61b8928b721c84d949fee07fd91edaf3198cdcdc2ff4","schema_version":"1.0","event_id":"sha256:2bd1bc45c914d423fa8e61b8928b721c84d949fee07fd91edaf3198cdcdc2ff4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/bundle.json","state_url":"https://pith.science/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/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":"2026-06-02T22:20:07Z","links":{"resolver":"https://pith.science/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY","bundle":"https://pith.science/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/bundle.json","state":"https://pith.science/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/65LGXCU7ZK6MGDMUTC3OX3U3IY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:65LGXCU7ZK6MGDMUTC3OX3U3IY","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":"90d4396f721099807f066910861910c3f875b8ddd22f13bfb5d5c2cfaa526610","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-07-23T02:23:37Z","title_canon_sha256":"220b0ad080064dd56d1ae305e4d0ae52376f0595553394fa5f011e3aa4420863"},"schema_version":"1.0","source":{"id":"1207.5279","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5279","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5279v3","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5279","created_at":"2026-05-18T01:56:15Z"},{"alias_kind":"pith_short_12","alias_value":"65LGXCU7ZK6M","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_16","alias_value":"65LGXCU7ZK6MGDMU","created_at":"2026-05-18T12:26:56Z"},{"alias_kind":"pith_short_8","alias_value":"65LGXCU7","created_at":"2026-05-18T12:26:56Z"}],"graph_snapshots":[{"event_id":"sha256:2bd1bc45c914d423fa8e61b8928b721c84d949fee07fd91edaf3198cdcdc2ff4","target":"graph","created_at":"2026-05-18T01:56:15Z","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 have applied the coupled-channel complex scaling method (ccCSM) to K^{bar}N-\\pi Y system. One advantage of ccCSM is that resonant states as well as scattering states can be treated in the same framework. For the interactions in the system, we have constructed a meson-baryon potential-matrix by basing on the chiral SU(3) theory and respecting the K^{bar}N scattering length obtained in the Martin's analysis. For future purpose to apply it more complicated system such as K^{bar}NN, we adopt a local Gaussian form in the r-space. We have investigated both the non-relativistic (NR) and the semi-r","authors_text":"Akinobu Dote, Takashi Inoue, Takayuki Myo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-07-23T02:23:37Z","title":"Comprehensive application of a coupled-channel complex scaling method to the KbarN-piY system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5279","kind":"arxiv","version":3},"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:d470160dc76cf28ab58df64a99980a4fbed158dad64f552ed8b6b9b68d64f296","target":"record","created_at":"2026-05-18T01:56:15Z","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":"90d4396f721099807f066910861910c3f875b8ddd22f13bfb5d5c2cfaa526610","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-07-23T02:23:37Z","title_canon_sha256":"220b0ad080064dd56d1ae305e4d0ae52376f0595553394fa5f011e3aa4420863"},"schema_version":"1.0","source":{"id":"1207.5279","kind":"arxiv","version":3}},"canonical_sha256":"f7566b8a9fcabcc30d9498b6ebee9b460c1ff296ef42ab1239cbd5ab47525566","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f7566b8a9fcabcc30d9498b6ebee9b460c1ff296ef42ab1239cbd5ab47525566","first_computed_at":"2026-05-18T01:56:15.163679Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:56:15.163679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XmFihnch21E2jE5fk2SFl60fjpCGCixXmmq6MY0423ra1CDsvdCQU/bxh7gml9Bu7sRMnpT+y84GjmlD8vpCAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:56:15.164269Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.5279","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d470160dc76cf28ab58df64a99980a4fbed158dad64f552ed8b6b9b68d64f296","sha256:2bd1bc45c914d423fa8e61b8928b721c84d949fee07fd91edaf3198cdcdc2ff4"],"state_sha256":"36864ab8eaa5a4ba50770cd0c68bba7e3e926798d36a18f243bab37e394f23b3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0OGvdKuRa/ytkj9APaSQthsUBqXWrKD31crnw300y0KzeUJzaIxhuYHfyojGZH9d2lsiQkcUWhxOwWFQnSMMAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T22:20:07.912739Z","bundle_sha256":"5c08e7d6a17bbee6d047177a207cb36654596a1ca9e9941f49773602136332ff"}}