{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:GPKYYR6IW7OJWFUOY2FPRMUT5T","short_pith_number":"pith:GPKYYR6I","canonical_record":{"source":{"id":"1611.09025","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-28T08:47:38Z","cross_cats_sorted":[],"title_canon_sha256":"2adb547a42dda77d70d28e3cf1cf9d7ceca89ab065953be17bb5425455288912","abstract_canon_sha256":"52f86ab1053b052b07f85195d5f4f196c7d12e4186ae6b0135ed4c8e287c068d"},"schema_version":"1.0"},"canonical_sha256":"33d58c47c8b7dc9b168ec68af8b293ecdcd44b993398e38f60bc70da4a17d725","source":{"kind":"arxiv","id":"1611.09025","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.09025","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"arxiv_version","alias_value":"1611.09025v1","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.09025","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"pith_short_12","alias_value":"GPKYYR6IW7OJ","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_16","alias_value":"GPKYYR6IW7OJWFUO","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_8","alias_value":"GPKYYR6I","created_at":"2026-05-18T12:30:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:GPKYYR6IW7OJWFUOY2FPRMUT5T","target":"record","payload":{"canonical_record":{"source":{"id":"1611.09025","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-28T08:47:38Z","cross_cats_sorted":[],"title_canon_sha256":"2adb547a42dda77d70d28e3cf1cf9d7ceca89ab065953be17bb5425455288912","abstract_canon_sha256":"52f86ab1053b052b07f85195d5f4f196c7d12e4186ae6b0135ed4c8e287c068d"},"schema_version":"1.0"},"canonical_sha256":"33d58c47c8b7dc9b168ec68af8b293ecdcd44b993398e38f60bc70da4a17d725","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:56:29.459770Z","signature_b64":"ku8vpGxJH4WNhhgyDrdUtAKgUJ7L6sq+fZ9xgV3REESxKtZeaakFWm5BiXsxbt+W04hfmacQssslof6XW3eYBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33d58c47c8b7dc9b168ec68af8b293ecdcd44b993398e38f60bc70da4a17d725","last_reissued_at":"2026-05-18T00:56:29.459086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:56:29.459086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.09025","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":"2026-05-18T00:56:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TbYea7sZ8fvmSMCWHF0q+aJWJHbXS+yJ2eVW6X0mwhvLV3fiXotqoLIdLb4ulw6lJgmsO2+lhoAj6sNfy+cADA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T18:47:59.095059Z"},"content_sha256":"af13546ed4e9089a70afcc54f47c341b7bb927e208d86f034fc24da5bb1b269a","schema_version":"1.0","event_id":"sha256:af13546ed4e9089a70afcc54f47c341b7bb927e208d86f034fc24da5bb1b269a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:GPKYYR6IW7OJWFUOY2FPRMUT5T","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coupled-channels Faddeev AGS calculation of $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"S. Marri, S. Z. Kalantari","submitted_at":"2016-11-28T08:47:38Z","abstract_excerpt":"Using separable $\\bar{K}N-\\pi\\Sigma$ potentials in the Faddeev equations, we calculated the binding energies and widths of the $K^{-}pp$, $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states on the basis of three- and four-body Alt-Grassberger-Sandhas equations in the momentum representation. One- and two-pole version of $\\bar{K}N-\\pi\\Sigma$ interaction are considered and the dependence of the resulting few-body energy on the two-body $\\bar{K}N-\\pi\\Sigma$ potential was investigated. The $s$-wave [3+1] and [2+2] sub-amplitudes are obtained by using the Hilbert-Schmidt expansion procedure for the integr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.09025","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":"2026-05-18T00:56:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F39gfncIgJamzAcUqXHH3tQPPlJVr+kcQ02d3jp7U6ynVtcFvumBAaTZbbCmkilpJnMaKW31sJnBggI3rBk3DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T18:47:59.095704Z"},"content_sha256":"81d94052af0b2209b7a4bf466b79ba5b59d56fbfc1840e06c1b4defdab9ae9ea","schema_version":"1.0","event_id":"sha256:81d94052af0b2209b7a4bf466b79ba5b59d56fbfc1840e06c1b4defdab9ae9ea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/bundle.json","state_url":"https://pith.science/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/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":"2026-06-05T18:47:59Z","links":{"resolver":"https://pith.science/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T","bundle":"https://pith.science/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/bundle.json","state":"https://pith.science/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GPKYYR6IW7OJWFUOY2FPRMUT5T/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:GPKYYR6IW7OJWFUOY2FPRMUT5T","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":"52f86ab1053b052b07f85195d5f4f196c7d12e4186ae6b0135ed4c8e287c068d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-28T08:47:38Z","title_canon_sha256":"2adb547a42dda77d70d28e3cf1cf9d7ceca89ab065953be17bb5425455288912"},"schema_version":"1.0","source":{"id":"1611.09025","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.09025","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"arxiv_version","alias_value":"1611.09025v1","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.09025","created_at":"2026-05-18T00:56:29Z"},{"alias_kind":"pith_short_12","alias_value":"GPKYYR6IW7OJ","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_16","alias_value":"GPKYYR6IW7OJWFUO","created_at":"2026-05-18T12:30:19Z"},{"alias_kind":"pith_short_8","alias_value":"GPKYYR6I","created_at":"2026-05-18T12:30:19Z"}],"graph_snapshots":[{"event_id":"sha256:81d94052af0b2209b7a4bf466b79ba5b59d56fbfc1840e06c1b4defdab9ae9ea","target":"graph","created_at":"2026-05-18T00:56:29Z","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":"Using separable $\\bar{K}N-\\pi\\Sigma$ potentials in the Faddeev equations, we calculated the binding energies and widths of the $K^{-}pp$, $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states on the basis of three- and four-body Alt-Grassberger-Sandhas equations in the momentum representation. One- and two-pole version of $\\bar{K}N-\\pi\\Sigma$ interaction are considered and the dependence of the resulting few-body energy on the two-body $\\bar{K}N-\\pi\\Sigma$ potential was investigated. The $s$-wave [3+1] and [2+2] sub-amplitudes are obtained by using the Hilbert-Schmidt expansion procedure for the integr","authors_text":"S. Marri, S. Z. Kalantari","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-28T08:47:38Z","title":"Coupled-channels Faddeev AGS calculation of $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.09025","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:af13546ed4e9089a70afcc54f47c341b7bb927e208d86f034fc24da5bb1b269a","target":"record","created_at":"2026-05-18T00:56:29Z","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":"52f86ab1053b052b07f85195d5f4f196c7d12e4186ae6b0135ed4c8e287c068d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-28T08:47:38Z","title_canon_sha256":"2adb547a42dda77d70d28e3cf1cf9d7ceca89ab065953be17bb5425455288912"},"schema_version":"1.0","source":{"id":"1611.09025","kind":"arxiv","version":1}},"canonical_sha256":"33d58c47c8b7dc9b168ec68af8b293ecdcd44b993398e38f60bc70da4a17d725","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"33d58c47c8b7dc9b168ec68af8b293ecdcd44b993398e38f60bc70da4a17d725","first_computed_at":"2026-05-18T00:56:29.459086Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:56:29.459086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ku8vpGxJH4WNhhgyDrdUtAKgUJ7L6sq+fZ9xgV3REESxKtZeaakFWm5BiXsxbt+W04hfmacQssslof6XW3eYBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:56:29.459770Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.09025","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:af13546ed4e9089a70afcc54f47c341b7bb927e208d86f034fc24da5bb1b269a","sha256:81d94052af0b2209b7a4bf466b79ba5b59d56fbfc1840e06c1b4defdab9ae9ea"],"state_sha256":"08f62ab9d4dd97c38f4461b70697cfb0fa590c031906ba125f67b7d7579b29cf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jCYSadDVvL8K6LVikfbFJ/G/W2v78KaztE6n4tsP5o+VB7tKQ0fgUrG4SpRG5L2t1ro41MGvjIl6q3YNw+TEBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T18:47:59.098935Z","bundle_sha256":"aa7c27ef0178e81d68caeaac3a008acee1bf0ad71e47dc56f1313c90131e5b8f"}}