{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:RHIPGACD2XHCG24FMSJZQVVXIE","short_pith_number":"pith:RHIPGACD","canonical_record":{"source":{"id":"1806.05651","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T17:07:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d9cd9111bf84628dcbcc9df8fffac6ae291df7621bce3828eb6fc9173043e60c","abstract_canon_sha256":"84541d2e9ba79547f04bdc2ed4e1817ec70b4f3a987f222c0949ba666431152c"},"schema_version":"1.0"},"canonical_sha256":"89d0f30043d5ce236b8564939856b741355be624eef7ce1e6661e706abec693f","source":{"kind":"arxiv","id":"1806.05651","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.05651","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"arxiv_version","alias_value":"1806.05651v2","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.05651","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"pith_short_12","alias_value":"RHIPGACD2XHC","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RHIPGACD2XHCG24F","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RHIPGACD","created_at":"2026-05-18T12:32:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:RHIPGACD2XHCG24FMSJZQVVXIE","target":"record","payload":{"canonical_record":{"source":{"id":"1806.05651","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T17:07:36Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"d9cd9111bf84628dcbcc9df8fffac6ae291df7621bce3828eb6fc9173043e60c","abstract_canon_sha256":"84541d2e9ba79547f04bdc2ed4e1817ec70b4f3a987f222c0949ba666431152c"},"schema_version":"1.0"},"canonical_sha256":"89d0f30043d5ce236b8564939856b741355be624eef7ce1e6661e706abec693f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:59.353483Z","signature_b64":"T+lOM3OqEOb/+hLdMcbjre3pqPfYi/zEluX/KR7MKx4MU9QIjZNXlNYP9VkURg2FPgR8zRFs7szM/IB8MdCDAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89d0f30043d5ce236b8564939856b741355be624eef7ce1e6661e706abec693f","last_reissued_at":"2026-05-18T00:06:59.352752Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:59.352752Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1806.05651","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:06:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D7t7NK07igsTPeN9kJTYF4BWBlzN/uNUIoSBRPe1cjNtlsQtQ257aFKqk1nlKuGD8md5psRuvK0CCShy+AV3BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:31:57.152008Z"},"content_sha256":"aa84907a0897c10b841c44cdd2fe9bb781519d133891895dfdcace2a4bd2175c","schema_version":"1.0","event_id":"sha256:aa84907a0897c10b841c44cdd2fe9bb781519d133891895dfdcace2a4bd2175c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:RHIPGACD2XHCG24FMSJZQVVXIE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Radiative and $\\rho$ transitions between heavy quarkonium and isovector four-quark states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"M.B. Voloshin","submitted_at":"2018-06-14T17:07:36Z","abstract_excerpt":"The recent observation and measurement of the decay $Z_c(3900) \\to \\rho \\eta_c$ provides the data on the relative strength of the pion and $\\rho$ coupling in the corresponding transitions between exotic resonances and pure heavy quarkonium. It is argued that using these data, the heavy quark limit for the $c$ and $b$ quarks, the heavy quark spin symmetry (HQSS) and the vector dominance for photon emission by the light quarks, one can (approximately) quantitatively estimate the rates of the radiative transitions from $\\Upsilon(5S)$ to the expected $G$-odd states of molecular bottomonium $W_{bJ}"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.05651","kind":"arxiv","version":2},"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":"2026-05-18T00:06:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EpONsgHjRiVz/QX2ECY6lhOjHxi1wq938jnadC1vuntnGOohTZFCIJqOf3jU77RX4BuzRWlOtPLmJBuenr4iBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:31:57.152379Z"},"content_sha256":"6f135330cd8d74c56f62b778ab5e4b316f07fc8fd483e8143616ea97c6d95f08","schema_version":"1.0","event_id":"sha256:6f135330cd8d74c56f62b778ab5e4b316f07fc8fd483e8143616ea97c6d95f08"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RHIPGACD2XHCG24FMSJZQVVXIE/bundle.json","state_url":"https://pith.science/pith/RHIPGACD2XHCG24FMSJZQVVXIE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RHIPGACD2XHCG24FMSJZQVVXIE/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":"2026-06-01T06:31:57Z","links":{"resolver":"https://pith.science/pith/RHIPGACD2XHCG24FMSJZQVVXIE","bundle":"https://pith.science/pith/RHIPGACD2XHCG24FMSJZQVVXIE/bundle.json","state":"https://pith.science/pith/RHIPGACD2XHCG24FMSJZQVVXIE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RHIPGACD2XHCG24FMSJZQVVXIE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RHIPGACD2XHCG24FMSJZQVVXIE","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":"84541d2e9ba79547f04bdc2ed4e1817ec70b4f3a987f222c0949ba666431152c","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T17:07:36Z","title_canon_sha256":"d9cd9111bf84628dcbcc9df8fffac6ae291df7621bce3828eb6fc9173043e60c"},"schema_version":"1.0","source":{"id":"1806.05651","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1806.05651","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"arxiv_version","alias_value":"1806.05651v2","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.05651","created_at":"2026-05-18T00:06:59Z"},{"alias_kind":"pith_short_12","alias_value":"RHIPGACD2XHC","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RHIPGACD2XHCG24F","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RHIPGACD","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:6f135330cd8d74c56f62b778ab5e4b316f07fc8fd483e8143616ea97c6d95f08","target":"graph","created_at":"2026-05-18T00:06:59Z","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 recent observation and measurement of the decay $Z_c(3900) \\to \\rho \\eta_c$ provides the data on the relative strength of the pion and $\\rho$ coupling in the corresponding transitions between exotic resonances and pure heavy quarkonium. It is argued that using these data, the heavy quark limit for the $c$ and $b$ quarks, the heavy quark spin symmetry (HQSS) and the vector dominance for photon emission by the light quarks, one can (approximately) quantitatively estimate the rates of the radiative transitions from $\\Upsilon(5S)$ to the expected $G$-odd states of molecular bottomonium $W_{bJ}","authors_text":"M.B. Voloshin","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T17:07:36Z","title":"Radiative and $\\rho$ transitions between heavy quarkonium and isovector four-quark states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.05651","kind":"arxiv","version":2},"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:aa84907a0897c10b841c44cdd2fe9bb781519d133891895dfdcace2a4bd2175c","target":"record","created_at":"2026-05-18T00:06:59Z","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":"84541d2e9ba79547f04bdc2ed4e1817ec70b4f3a987f222c0949ba666431152c","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T17:07:36Z","title_canon_sha256":"d9cd9111bf84628dcbcc9df8fffac6ae291df7621bce3828eb6fc9173043e60c"},"schema_version":"1.0","source":{"id":"1806.05651","kind":"arxiv","version":2}},"canonical_sha256":"89d0f30043d5ce236b8564939856b741355be624eef7ce1e6661e706abec693f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89d0f30043d5ce236b8564939856b741355be624eef7ce1e6661e706abec693f","first_computed_at":"2026-05-18T00:06:59.352752Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:06:59.352752Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"T+lOM3OqEOb/+hLdMcbjre3pqPfYi/zEluX/KR7MKx4MU9QIjZNXlNYP9VkURg2FPgR8zRFs7szM/IB8MdCDAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:06:59.353483Z","signed_message":"canonical_sha256_bytes"},"source_id":"1806.05651","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:aa84907a0897c10b841c44cdd2fe9bb781519d133891895dfdcace2a4bd2175c","sha256:6f135330cd8d74c56f62b778ab5e4b316f07fc8fd483e8143616ea97c6d95f08"],"state_sha256":"b22534b7d2fcf831c602c3cfe48ceb5c6a8f5a05a94dbca5071e7745de030717"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q0yl6UMizVYqyot5IY5DLqa3MiGoO3k/7XkTQe9UHotFJnh9WpMj3iZisRGhY46ekPxsl77p+OU2JSR15gYYBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T06:31:57.154369Z","bundle_sha256":"5c0ac30ceab43141f0ad7d42068f4593c408991ab4d82762fd92d0f96f2d8e35"}}