{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:3SQHGEHKUMKUBVILL5U5JPA55Q","short_pith_number":"pith:3SQHGEHK","canonical_record":{"source":{"id":"1705.09631","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-26T16:03:14Z","cross_cats_sorted":[],"title_canon_sha256":"cb0e1eeb91d987fb653ca1ce3a87718a873855288915c494797e11bdb3b748d4","abstract_canon_sha256":"c5a572a90956e4d553d348ef68e1d0c8fc3dbf6057c6dcb859560773c71fafc3"},"schema_version":"1.0"},"canonical_sha256":"dca07310eaa31540d50b5f69d4bc1dec1f58ff91559e80bcf573de264acba5cc","source":{"kind":"arxiv","id":"1705.09631","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.09631","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"arxiv_version","alias_value":"1705.09631v3","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.09631","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"pith_short_12","alias_value":"3SQHGEHKUMKU","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3SQHGEHKUMKUBVIL","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3SQHGEHK","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:3SQHGEHKUMKUBVILL5U5JPA55Q","target":"record","payload":{"canonical_record":{"source":{"id":"1705.09631","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-26T16:03:14Z","cross_cats_sorted":[],"title_canon_sha256":"cb0e1eeb91d987fb653ca1ce3a87718a873855288915c494797e11bdb3b748d4","abstract_canon_sha256":"c5a572a90956e4d553d348ef68e1d0c8fc3dbf6057c6dcb859560773c71fafc3"},"schema_version":"1.0"},"canonical_sha256":"dca07310eaa31540d50b5f69d4bc1dec1f58ff91559e80bcf573de264acba5cc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:58.811941Z","signature_b64":"lPSp38Wiej+tsH+iDIaKecTY97W1bQib2h0Bq5jsZldR66PyvRcMaZMXaIL9X/ck40083gY5weEbj1CkFiqmAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dca07310eaa31540d50b5f69d4bc1dec1f58ff91559e80bcf573de264acba5cc","last_reissued_at":"2026-05-18T00:31:58.811569Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:58.811569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.09631","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":"2026-05-18T00:31:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0rDJap8/qVTuFAYdzSvTwKBmZd439dtX6tewgvq+wc4i8YZHiRTVqH3njxLa2LTBs4YfxzAkYt+s0psvEzTvAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T13:05:53.401805Z"},"content_sha256":"4376b1290a52c4e6d28ee4b6af5532c61fc4266adf0729fc3edb9e3cd80f7e39","schema_version":"1.0","event_id":"sha256:4376b1290a52c4e6d28ee4b6af5532c61fc4266adf0729fc3edb9e3cd80f7e39"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:3SQHGEHKUMKUBVILL5U5JPA55Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Selected strong decays of $\\eta(2225)$ and $\\phi(2170)$ as $\\Lambda \\bar\\Lambda$ bound states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Amand Faessler, Qifang L\\\"u, Thomas Gutsche, Valery E. Lyubovitskij, Yubing Dong","submitted_at":"2017-05-26T16:03:14Z","abstract_excerpt":"The strong decays of the two resonances $\\eta(2225)$ and $\\phi(2170)$ are discussed for selected decay channels. The two resonances are considered as the $\\Lambda \\bar{\\Lambda}$ bound states in the molecular scenario. The phenomenological hadronic molecular approach is employed for the calculation of respective decay modes using effective Lagrangians. Our results show that the decay modes $\\eta(2225)\\to K^*K$ and $\\phi(2175) \\to KK$ dominate over the partial decay widths of $\\eta(2275)\\to VV (\\phi\\phi, \\omega\\omega, K^*K^*)$ and $\\phi(2175)\\to VS (\\omega\\sigma, K^*K^*_0(800), \\phi f_0(980))$ d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.09631","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":"2026-05-18T00:31:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+NB5dkekagARd5EgWKNbJozX9UDfD6+PNzkrUNaBWRr4D/kbjTaYQTHp0NWzSGJ/9+GdkRovona2BS/escvoAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T13:05:53.402153Z"},"content_sha256":"d193ca560204a6a1cfd771c9a96aee9936e0ca3eb3c0607ed3a9d4d6cace230e","schema_version":"1.0","event_id":"sha256:d193ca560204a6a1cfd771c9a96aee9936e0ca3eb3c0607ed3a9d4d6cace230e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/bundle.json","state_url":"https://pith.science/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/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":"2026-06-11T13:05:53Z","links":{"resolver":"https://pith.science/pith/3SQHGEHKUMKUBVILL5U5JPA55Q","bundle":"https://pith.science/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/bundle.json","state":"https://pith.science/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3SQHGEHKUMKUBVILL5U5JPA55Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:3SQHGEHKUMKUBVILL5U5JPA55Q","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":"c5a572a90956e4d553d348ef68e1d0c8fc3dbf6057c6dcb859560773c71fafc3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-26T16:03:14Z","title_canon_sha256":"cb0e1eeb91d987fb653ca1ce3a87718a873855288915c494797e11bdb3b748d4"},"schema_version":"1.0","source":{"id":"1705.09631","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.09631","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"arxiv_version","alias_value":"1705.09631v3","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.09631","created_at":"2026-05-18T00:31:58Z"},{"alias_kind":"pith_short_12","alias_value":"3SQHGEHKUMKU","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3SQHGEHKUMKUBVIL","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3SQHGEHK","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:d193ca560204a6a1cfd771c9a96aee9936e0ca3eb3c0607ed3a9d4d6cace230e","target":"graph","created_at":"2026-05-18T00:31:58Z","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 strong decays of the two resonances $\\eta(2225)$ and $\\phi(2170)$ are discussed for selected decay channels. The two resonances are considered as the $\\Lambda \\bar{\\Lambda}$ bound states in the molecular scenario. The phenomenological hadronic molecular approach is employed for the calculation of respective decay modes using effective Lagrangians. Our results show that the decay modes $\\eta(2225)\\to K^*K$ and $\\phi(2175) \\to KK$ dominate over the partial decay widths of $\\eta(2275)\\to VV (\\phi\\phi, \\omega\\omega, K^*K^*)$ and $\\phi(2175)\\to VS (\\omega\\sigma, K^*K^*_0(800), \\phi f_0(980))$ d","authors_text":"Amand Faessler, Qifang L\\\"u, Thomas Gutsche, Valery E. Lyubovitskij, Yubing Dong","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-26T16:03:14Z","title":"Selected strong decays of $\\eta(2225)$ and $\\phi(2170)$ as $\\Lambda \\bar\\Lambda$ bound states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.09631","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":"sha256:4376b1290a52c4e6d28ee4b6af5532c61fc4266adf0729fc3edb9e3cd80f7e39","target":"record","created_at":"2026-05-18T00:31:58Z","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":"c5a572a90956e4d553d348ef68e1d0c8fc3dbf6057c6dcb859560773c71fafc3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-05-26T16:03:14Z","title_canon_sha256":"cb0e1eeb91d987fb653ca1ce3a87718a873855288915c494797e11bdb3b748d4"},"schema_version":"1.0","source":{"id":"1705.09631","kind":"arxiv","version":3}},"canonical_sha256":"dca07310eaa31540d50b5f69d4bc1dec1f58ff91559e80bcf573de264acba5cc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dca07310eaa31540d50b5f69d4bc1dec1f58ff91559e80bcf573de264acba5cc","first_computed_at":"2026-05-18T00:31:58.811569Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:31:58.811569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lPSp38Wiej+tsH+iDIaKecTY97W1bQib2h0Bq5jsZldR66PyvRcMaZMXaIL9X/ck40083gY5weEbj1CkFiqmAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:31:58.811941Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.09631","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4376b1290a52c4e6d28ee4b6af5532c61fc4266adf0729fc3edb9e3cd80f7e39","sha256:d193ca560204a6a1cfd771c9a96aee9936e0ca3eb3c0607ed3a9d4d6cace230e"],"state_sha256":"b0f0b7f2787f2a72531c6c79913619005e51d0bf46e3064c16fdab8e33350753"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FcENMqAYnVZnP4Yd4W7SsWlHwtuSpSWHzLaz+6Piylqeh6+SzR1zdofD1bTz796XmW79gM5vFi3cydA908neAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T13:05:53.404108Z","bundle_sha256":"e80a42372cbc7ed9bcaea5ed56e5f2a94053443577e607c063204a31b0d88c11"}}