{"as_of":"2026-08-07T17:37:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6d1bbec30d07f8f5db3005750e8a4694fa7d7ab8468fc0940b09c0da766c1589","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":59,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":59,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-07T06:34:17.273281+00:00","state":"measured"},{"denominator":59,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":59,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T15:10:21.819751Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-04T19:20:06.764974Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2411.15689","last_updated":"2026-03-03T04:11:30Z","snapshot_observed_at":"2026-07-06T19:56:04.259325Z","submitted_at":"2024-11-24T02:30:01Z","title":"Prospects for observing the missing $2D$ and $1F$ charmonium states around 4 GeV","version":5},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-23T17:23:11.118998Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2411.15689"},"observation_digest":"sha256:27d911009df8db467ddb2795cb8970a71e7200dbb0362ac35de8af0b87ff5595","observation_id":"195272c2-2c8a-481c-9c1b-78ee7d884f45","resolution":{"observed_at":"2026-05-23T17:23:14.915040Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2502.15117","last_updated":"2026-04-04T01:29:30Z","snapshot_observed_at":"2026-08-03T21:56:54.106294Z","submitted_at":"2025-02-21T00:37:08Z","title":"Colloquium: Hadron Production in Open-charm Meson Pair at $e^+e^-$ Collider","version":4},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-23T03:05:07.109776Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2502.15117"},"observation_digest":"sha256:fe88da3223a07d21c27000f77ae5d604f33a0114d90fe3a0457ff6ba8b716324","observation_id":"46384bac-67d1-40fe-8101-93aaac273f39","resolution":{"observed_at":"2026-05-23T03:05:20.175048Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-07T15:10:21.819751Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.16219","last_updated":"2025-05-22T04:43:39Z","snapshot_observed_at":"2026-08-07T15:03:03.734909Z","submitted_at":"2025-05-22T04:43:39Z","title":"Hidden-Charm Tetraquarks in a Mixture Model: Coupled-Channel Analysis with $c\\bar{c}$ and Hadronic Molecular Components","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-07T15:10:21.819751Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2505.16219"},"observation_digest":"sha256:ccef7045ddd46bb47dc1b208439d58acb7a64ad075d1181b3954a0f3da6e3ff8","observation_id":"76d214f7-1534-4305-87d8-0eebd8b0b0ba","resolution":{"observed_at":"2026-08-07T15:10:21.819751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-07T13:22:50.028048Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.22177","last_updated":"2025-05-28T09:52:04Z","snapshot_observed_at":"2026-08-07T13:10:59.424534Z","submitted_at":"2025-05-28T09:52:04Z","title":"Hydrogen-like structures in the strong interaction","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-07T13:22:50.028048Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2505.22177"},"observation_digest":"sha256:554a66d9d8bef979343d3d4e7eb3004bf1f396bb22c92d0b1373da87d12d111c","observation_id":"96e72f98-5bf9-4873-bb1b-6775ee6d41e0","resolution":{"observed_at":"2026-08-07T13:22:50.028048Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-07T10:55:48.079401Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.04345","last_updated":"2025-06-13T20:07:14Z","snapshot_observed_at":"2026-08-07T10:41:56.272837Z","submitted_at":"2025-06-04T18:02:33Z","title":"Probing the electromagnetic structure of the $P_c(4337)^+$ pentaquark: Insights from a diquark-diquark-antiquark picture for $J^P = \\frac{1}{2}^-$ and $\\frac{3}{2}^-$ states","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-07T10:55:48.079401Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2506.04345"},"observation_digest":"sha256:58dc167ec7d0e1836b19eaed12c8ac3a22c9f2628bce3809c867bebc6730f6a7","observation_id":"f64d51aa-99a7-47c3-9a9e-fb1fcf65bdff","resolution":{"observed_at":"2026-08-07T10:55:48.079401Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-07T00:25:35.476165Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.14527","last_updated":"2025-06-23T12:15:15Z","snapshot_observed_at":"2026-08-07T04:16:22.742437Z","submitted_at":"2025-06-17T13:52:45Z","title":"Scalar Triple-Heavy Tetraquark States With Quark Content $cc\\bar{c}\\bar{s}$","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-07T00:25:35.476165Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2506.14527"},"observation_digest":"sha256:cd6588055932b2f4281391c17f5fd376d92f361e91661d3691e2816de9723760","observation_id":"85f60166-23ae-4839-8606-cbb51e9d5b3a","resolution":{"observed_at":"2026-08-07T00:25:35.476165Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T23:55:49.622702Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.15584","last_updated":"2026-07-13T10:10:31Z","snapshot_observed_at":"2026-08-06T23:50:24.154656Z","submitted_at":"2025-06-18T16:00:35Z","title":"Charm physics","version":2},"reference_index":188,"source":"pdf_text","source_observed_at":"2026-08-06T23:55:49.622702Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2506.15584"},"observation_digest":"sha256:cfbced36c4c2311490319a1b415de80939ef702d4f77bb95650b646ffbe5f6b5","observation_id":"7d4ae618-28b8-4d04-823a-8683f37f9a32","resolution":{"observed_at":"2026-08-06T23:55:49.622702Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T22:24:48.542242Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.21949","last_updated":"2025-06-27T06:44:38Z","snapshot_observed_at":"2026-08-07T14:00:53.271408Z","submitted_at":"2025-06-27T06:44:38Z","title":"Eigenstates in coupled-channel scattering amplitude and their effects on spectrum","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T22:24:48.542242Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2506.21949"},"observation_digest":"sha256:2676b006b42963ebbaa2ba1e7954aca5d940deec9ae678b3f9c15e3ce2e17248","observation_id":"49a83269-c2f0-4828-8af7-3c0712598335","resolution":{"observed_at":"2026-08-06T22:24:48.542242Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T21:47:55.630787Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23476","last_updated":"2026-05-26T16:15:23Z","snapshot_observed_at":"2026-08-06T21:38:57.228294Z","submitted_at":"2025-06-30T02:42:57Z","title":"Probing the structure of the $D_{s 0}^*(2317)$ and $X(3872)$ states through correlation functions","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T21:47:55.630787Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2506.23476"},"observation_digest":"sha256:6ced462daa4c70166a1576d2124337706f67e76e1deae65ba379fbe68b603154","observation_id":"b33fd9a0-e61d-4b89-a90e-f02dc28548da","resolution":{"observed_at":"2026-08-06T21:47:55.630787Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T19:47:25.349445Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.04835","last_updated":"2026-06-10T09:30:27Z","snapshot_observed_at":"2026-08-06T23:27:47.889586Z","submitted_at":"2025-07-07T09:57:51Z","title":"Cross section of the process $e^+ + e^- \\to \\Xi^0 + \\bar{\\Xi}^0$ in the vicinity of charmonium $\\psi(3770)$ and in the charmonium (-like) state including the $D$-meson loop and three-gluon contributions","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T19:47:25.349445Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2507.04835"},"observation_digest":"sha256:354346a631a612bca291b7f81a80792099d04e00c5ee45586c41936a97a2bf74","observation_id":"15c94de4-0506-4ece-a022-0934e9eca8b8","resolution":{"observed_at":"2026-08-06T19:47:25.349445Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T16:21:41.782538Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.13882","last_updated":"2025-07-18T12:59:31Z","snapshot_observed_at":"2026-08-06T23:28:25.505171Z","submitted_at":"2025-07-18T12:59:31Z","title":"$\\Upsilon(5S)$ in the unquenched quark model","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T16:21:41.782538Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2507.13882"},"observation_digest":"sha256:b43b4ef97298919588c0737a4cccd930379127560999531ce4c9d6e42d31af02","observation_id":"68d63e39-97e6-47b1-a62f-af3224f61866","resolution":{"observed_at":"2026-08-06T16:21:41.782538Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-06T13:19:17.067826Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.20821","last_updated":"2025-07-28T13:26:06Z","snapshot_observed_at":"2026-08-06T17:19:27.517393Z","submitted_at":"2025-07-28T13:26:06Z","title":"The Pattern of Exotic Hidden-Heavy Hadrons Revealed","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T13:19:17.067826Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2507.20821"},"observation_digest":"sha256:96c99332157cf93910ac3cca930e370a6ffc0099e257a2d86db56cf77021cf8c","observation_id":"e382fd27-bef4-4d7c-bf0b-f87e08a81bed","resolution":{"observed_at":"2026-08-06T13:19:17.067826Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2507.21672","last_updated":"2025-07-31T10:12:27Z","snapshot_observed_at":"2026-07-06T22:04:30.930113Z","submitted_at":"2025-07-29T10:31:35Z","title":"Hadronic Molecules and $\\chi_{cJ}(2P)$ Coupled States","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-19T03:21:18.843687Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2507.21672"},"observation_digest":"sha256:e78d8f8fac7a8ed75d11855fc5e628b18d6cb8c2920fb20384cbd023f371ae5b","observation_id":"36c01fb5-ba95-4d5c-a83f-25e2a07c3074","resolution":{"observed_at":"2026-05-19T03:22:00.784964Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-05T23:14:14.039773Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.05825","last_updated":"2025-08-07T20:04:38Z","snapshot_observed_at":"2026-08-05T23:14:10.170540Z","submitted_at":"2025-08-07T20:04:38Z","title":"Correlation functions for $n\\,\\bar{D}_{s1}(2460)$ and $n\\,\\bar{D}_{s1}(2536)$","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-05T23:14:14.039773Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2508.05825"},"observation_digest":"sha256:919a7853d5022d8823260dcfbc51f87f8a508f210358d94e02f784aa14d72c23","observation_id":"24481c35-88fd-4389-be79-60463b4a1ccb","resolution":{"observed_at":"2026-08-05T23:14:14.039773Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-05T21:26:42.230910Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.08690","last_updated":"2025-08-12T07:29:00Z","snapshot_observed_at":"2026-08-06T17:22:56.674622Z","submitted_at":"2025-08-12T07:29:00Z","title":"ZS-Puffin: Design, Modeling and Implementation of an Unmanned Aerial-Aquatic Vehicle with Amphibious Wings","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T21:26:42.230910Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2508.08690"},"observation_digest":"sha256:9837644b8274eedba9629b53425ad5f071bafd8ec170631b2922eb2399591d90","observation_id":"42acffe0-94ab-424a-9389-ff79e08e3221","resolution":{"observed_at":"2026-08-05T21:26:42.230910Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-05T14:59:39.983445Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.20667","last_updated":"2025-08-28T11:20:00Z","snapshot_observed_at":"2026-08-05T19:49:40.927135Z","submitted_at":"2025-08-28T11:20:00Z","title":"Heavy quarkonia and new hadrons with two heavy quarks","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-05T14:59:39.983445Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2508.20667"},"observation_digest":"sha256:fc9ad6682bbb85f000c786486b7f290424e4a414cfa6587bac94e2b9c13f4126","observation_id":"895253d6-b429-45b3-9c28-e09c187438fd","resolution":{"observed_at":"2026-08-05T14:59:39.983445Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-05T14:23:51.168330Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.21474","last_updated":"2025-09-08T10:50:00Z","snapshot_observed_at":"2026-08-06T07:27:32.810736Z","submitted_at":"2025-08-29T09:58:21Z","title":"Prediction of $QQqq\\bar{s}$ molecular pentaquarks within the extended local hidden gauge approach","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T14:23:51.168330Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2508.21474"},"observation_digest":"sha256:62b8683515f883d11756d676d28ddd3bdfb54d98ba00906daf5d35aec61cefd6","observation_id":"c538640d-3e25-458c-90df-e96e82fe7079","resolution":{"observed_at":"2026-08-05T14:23:51.168330Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-04T16:57:14.304195Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.11234","last_updated":"2026-05-25T07:46:39Z","snapshot_observed_at":"2026-08-04T17:52:02.782838Z","submitted_at":"2025-09-14T12:22:09Z","title":"Investigating the two-pion exchange of the double charm $DD^*$ chiral interactions and $T_{cc}$","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T16:57:14.304195Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2509.11234"},"observation_digest":"sha256:1951386f692a6d2a159968f5a2c08e0cf06934df1cfdf38fe5a1d7f462b534f1","observation_id":"a8654084-936c-4ace-8e10-b3974eaf80f1","resolution":{"observed_at":"2026-08-04T16:57:14.304195Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-04T12:55:39.555240Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.01564","last_updated":"2026-06-18T06:47:48Z","snapshot_observed_at":"2026-08-04T12:55:35.781866Z","submitted_at":"2025-10-02T01:21:48Z","title":"A Paradigm for the Coupled-Channel Origin of Resonances: the Exotic $T_{c\\bar{s}}$ in $D_{s1}(2460/2536)\\to D_s\\pi\\pi$","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T12:55:39.555240Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2510.01564"},"observation_digest":"sha256:8dc1f4833bdf4260a79c0b7968f25709c32d7350129be12ea74db55c8b148d01","observation_id":"c42076b8-a185-4ce9-82db-c471d72f81f4","resolution":{"observed_at":"2026-08-04T12:55:39.555240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2510.17549","last_updated":"2026-04-29T14:32:34Z","snapshot_observed_at":"2026-07-06T22:33:34.164422Z","submitted_at":"2025-10-20T13:58:04Z","title":"Electromagnetic form factors and structure of the $T_{bb}$ tetraquark from lattice QCD","version":4},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-18T06:17:42.390465Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2510.17549"},"observation_digest":"sha256:426c093cd0aaea0bf8d8a11909b030c88ddec38dfae67b15e049bd83b57fd2a1","observation_id":"78f031e0-16bc-4a30-bdf4-29f9de1e79d8","resolution":{"observed_at":"2026-05-18T06:20:58.821630Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2510.23468","last_updated":"2026-05-10T04:25:23Z","snapshot_observed_at":"2026-08-06T21:41:38.381587Z","submitted_at":"2025-10-27T16:06:44Z","title":"Model-independent mass determination of near-threshold states from short-range production","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-18T04:24:26.782789Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2510.23468"},"observation_digest":"sha256:294281d6f4d0b35d0b470e0ff342431dbe9e1cf56b782a33f1efd4d15b6d0f42","observation_id":"2659995e-dc4c-4fe1-a9f8-d5c024fcdc8b","resolution":{"observed_at":"2026-05-18T04:25:51.915477Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-03T21:17:24.998757Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2511.16052","last_updated":"2026-06-05T17:45:22Z","snapshot_observed_at":"2026-08-03T21:17:24.027506Z","submitted_at":"2025-11-20T05:12:57Z","title":"Electromagnetic form factors: A window into the $D\\Lambda_c$, $D^*\\Lambda_c$, and $D\\Lambda_c^*$ molecular structure","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T21:17:24.998757Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2511.16052"},"observation_digest":"sha256:86f3532e4b9c0568a848198cc6c6ef31118428d1985bbce60e8d6f2f8382da25","observation_id":"a296ef2e-3df6-4001-9b51-d779b4ca258c","resolution":{"observed_at":"2026-08-03T21:17:24.998757Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2511.22590","last_updated":"2026-05-10T04:55:58Z","snapshot_observed_at":"2026-08-01T17:00:03.251551Z","submitted_at":"2025-11-27T16:23:27Z","title":"Short-range production of three bottom mesons","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-17T04:22:04.116096Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2511.22590"},"observation_digest":"sha256:236f455d5e2bb3843c38e43692bd1cfd35ff654facbe6cfcacae1eaad2e2b9dc","observation_id":"07f774c8-256d-4866-9bfc-ea1c447cee48","resolution":{"observed_at":"2026-05-17T04:24:00.509940Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-03T12:00:02.019802Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.04989","last_updated":"2026-06-11T02:54:26Z","snapshot_observed_at":"2026-08-06T00:53:01.497101Z","submitted_at":"2026-01-08T14:46:27Z","title":"Effective Range Expansion with the Left-Hand Cut: Higher Order Improvements","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T12:00:02.019802Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2601.04989"},"observation_digest":"sha256:d28dce1c344dd4fc58c34519dc39d08ed2f74c940691f6d48cecfc45e4a060f9","observation_id":"9d6e95a0-9291-40c9-aa09-dac8a2a567d0","resolution":{"observed_at":"2026-08-03T12:00:02.019802Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-03T09:32:06.276181Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.13789","last_updated":"2026-06-10T03:25:01Z","snapshot_observed_at":"2026-08-03T09:32:04.828696Z","submitted_at":"2026-01-20T09:44:13Z","title":"The dynamically generated $h_1$ state by the $K^*\\bar{K}^*$ interaction and its $K_1(1270)\\bar{K}$ and $b_1(1235)\\pi$ decays","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T09:32:06.276181Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2601.13789"},"observation_digest":"sha256:65ec91c7378d1c4fbaa5c9d620763f5b845bffe51e3055a73ed2aaa523ca1a10","observation_id":"c48ac9eb-adf8-4b6a-aa72-14181bd4a8b1","resolution":{"observed_at":"2026-08-03T09:32:06.276181Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-03T01:09:35.494514Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.10638","last_updated":"2026-05-29T08:12:33Z","snapshot_observed_at":"2026-08-06T08:37:00.668445Z","submitted_at":"2026-02-11T08:39:23Z","title":"Structural dissection of hadronic molecules: The $D^{(*)}\\bar{K}^{(*)}$ family under QCD light-cone sum rules","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T01:09:35.494514Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2602.10638"},"observation_digest":"sha256:50a454fb5def065cd591dbde9a9caf55b060973e8ca5e4cee1e90f41817507f6","observation_id":"b216e75d-a9c4-4be6-9021-8f14a3f1eb94","resolution":{"observed_at":"2026-08-03T01:09:35.494514Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2602.19504","last_updated":"2026-05-22T13:14:31Z","snapshot_observed_at":"2026-07-06T22:46:45.213871Z","submitted_at":"2026-02-23T04:40:54Z","title":"Three-body molecular states composed of $D^{(*)}$ and two nucleons","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-25T07:05:51.561552Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2602.19504"},"observation_digest":"sha256:f2fe6f1dba6b39e72aa9b0651f27b2d39f08c6aa078eb55ab4bc7cf91fa8081a","observation_id":"edac1cf7-bec4-42d3-9a10-ebb3e651f689","resolution":{"observed_at":"2026-05-25T07:06:41.571634Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-02T21:37:01.083644Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.19887","last_updated":"2026-08-05T09:25:10Z","snapshot_observed_at":"2026-08-07T17:03:41.234166Z","submitted_at":"2026-02-23T14:31:47Z","title":"Unquenched Charmonium and Beyond","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T21:37:01.083644Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2602.19887"},"observation_digest":"sha256:23894f6dc98dbe95cb0079837024ccaae6788cecc84933dea74b4b87073ae39c","observation_id":"d8df2ab4-8146-4e0f-a10b-940c63589d1c","resolution":{"observed_at":"2026-08-02T21:37:01.083644Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-02T18:28:02.139933Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2603.11154","last_updated":"2026-07-20T11:45:42Z","snapshot_observed_at":"2026-08-06T04:52:17.074841Z","submitted_at":"2026-03-11T18:00:00Z","title":"Dispersive Analysis of $D$- and $B$-Meson Form Factors with Chiral and Heavy-Quark Constraints","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-02T18:28:02.139933Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2603.11154"},"observation_digest":"sha256:dd2375ebd17b56d180a10a7768d00613608a3ad2744f2ae20c14459afe920223","observation_id":"0292db91-c7ac-467e-befb-e1913fb5807a","resolution":{"observed_at":"2026-08-02T18:28:02.139933Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2603.11259","last_updated":"2026-05-22T11:55:05Z","snapshot_observed_at":"2026-08-06T11:51:20.182892Z","submitted_at":"2026-03-11T19:38:54Z","title":"Comprehensive Mass Predictions: From Triply Heavy Baryons to Pentaquarks","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-25T06:38:56.109134Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2603.11259"},"observation_digest":"sha256:31b35ca5aed7cec97ab69415d725c90a02e9d74d43d5e0e8957a67e2bfc7020a","observation_id":"0f6f6567-ad35-4cc5-a4ee-367fc8fe8dd8","resolution":{"observed_at":"2026-05-25T06:40:25.369174Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.04821","last_updated":"2026-04-18T15:27:20Z","snapshot_observed_at":"2026-07-06T22:53:41.734429Z","submitted_at":"2026-04-06T16:24:28Z","title":"Study of the molecular Properties of the $P_c$ and $P_{cs}$ States","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-05-10T20:30:25.241387Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.04821"},"observation_digest":"sha256:2fea90bc85c897f545b6ff33d7d332cdd420b6d8c30fe40c9366e0bb1d099db2","observation_id":"9f194a3d-2038-4ed4-bcc5-4d5f21acf239","resolution":{"observed_at":"2026-05-10T21:55:50.132704Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.04846","last_updated":"2026-04-06T16:46:36Z","snapshot_observed_at":"2026-07-06T22:53:41.734429Z","submitted_at":"2026-04-06T16:46:36Z","title":"$\\boldsymbol{B_c}$ Meson Spectroscopy from Bayesian MCMC: Probing Confinement and State Mixing","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-05-10T20:20:20.805723Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.04846"},"observation_digest":"sha256:afb821b03e56522f1700de6175dc8db28c5eb5a50a70017b265bbc67aecd2532","observation_id":"56f3ff03-4d63-473b-822d-9da22510348e","resolution":{"observed_at":"2026-05-10T22:00:48.688082Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.12603","last_updated":"2026-04-14T11:29:06Z","snapshot_observed_at":"2026-07-06T23:00:46.620106Z","submitted_at":"2026-04-14T11:29:06Z","title":"Open-flavor threshold effects on quarkonium spectrum in the BOEFT","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-05-10T15:34:03.514667Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.12603"},"observation_digest":"sha256:001b7c28f91bad1b638b1f1b8fe5864ffe0188b348e065718060127a22c67f88","observation_id":"8f163c24-b0f1-40b1-b14e-1e5a20cc5169","resolution":{"observed_at":"2026-05-11T10:16:06.452020Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.17813","last_updated":"2026-04-20T05:11:34Z","snapshot_observed_at":"2026-08-02T21:42:57.933652Z","submitted_at":"2026-04-20T05:11:34Z","title":"Compositeness of near-threshold eigenstates with Coulomb plus short-range interactions","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-10T04:57:00.554879Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.17813"},"observation_digest":"sha256:148ebed3c72641a68293d5e9bc865c1da194ad93118c16e4391a96c1003d43b5","observation_id":"7a086319-e1ef-42ca-b26f-d73a41f13f2e","resolution":{"observed_at":"2026-05-10T11:00:04.845749Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.18286","last_updated":"2026-04-20T13:57:59Z","snapshot_observed_at":"2026-07-06T23:05:13.178333Z","submitted_at":"2026-04-20T13:57:59Z","title":"Analysis of the $D_0^*(2300)$ resonance from lattice QCD under chiral symmetry","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-05-10T04:17:11.253967Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.18286"},"observation_digest":"sha256:8b50d637c7305ef4e5f5be8ae70cda04c01fb32bddaafe67cc5e6f115cdca550","observation_id":"ee775664-b5ed-4079-814a-eee4468a0fb5","resolution":{"observed_at":"2026-05-11T12:01:06.657350Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.20439","last_updated":"2026-04-22T11:00:28Z","snapshot_observed_at":"2026-07-06T23:06:55.880484Z","submitted_at":"2026-04-22T11:00:28Z","title":"QCD sum rule analysis of local meson-meson currents for the $K(1690)$ state","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-10T00:34:14.952092Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.20439"},"observation_digest":"sha256:ad5838f622221313a01941d94468a9b8fe22040cea2d40968529a5e19f4e30d9","observation_id":"7e58b4c0-4981-4d5e-9f0b-566c47a66d11","resolution":{"observed_at":"2026-05-10T00:34:47.518817Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.22719","last_updated":"2026-04-24T17:07:15Z","snapshot_observed_at":"2026-07-06T23:09:05.682387Z","submitted_at":"2026-04-24T17:07:15Z","title":"Mechanisms of high energy polarized photoproduction of $\\pi^{-}\\Delta^{++}$","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-05-08T11:08:00.727375Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.22719"},"observation_digest":"sha256:2638530e2d544423aca359a89567617957da5a0dc076624ecbcc9f5e2bc461f1","observation_id":"b4dd9a7b-bf77-48f8-b237-ca31a114e24d","resolution":{"observed_at":"2026-05-11T19:46:07.367114Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.23298","last_updated":"2026-04-25T13:27:00Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2026-04-25T13:27:00Z","title":"Coupled-channel study of the three-body $DDK$ and $D^{*}D^{*}K$","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-08T07:54:25.944851Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.23298"},"observation_digest":"sha256:49ba80c228ce7c48896f9ac6d0f1f536133249ff0895b9f49ffa502f1417d7d7","observation_id":"667230c6-ad7f-4bb0-872a-f7c61c391884","resolution":{"observed_at":"2026-05-11T20:46:15.938345Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2604.25607","last_updated":"2026-04-28T13:11:21Z","snapshot_observed_at":"2026-07-06T23:11:25.757664Z","submitted_at":"2026-04-28T13:11:21Z","title":"Determination of the $Z_c(3900)$ and the $Z_{cs}(3985)$ states from joint analysis of experimental and lattice data","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-07T15:58:57.306436Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2604.25607"},"observation_digest":"sha256:ea2d436664ae92fd1677d08c60c84463900826e3eaa8d8c5a0123f3a688b95d8","observation_id":"9f3a7fcd-0db3-49c0-a9ee-b74cae53e77b","resolution":{"observed_at":"2026-05-11T23:56:14.631856Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2605.01539","last_updated":"2026-07-06T16:58:43Z","snapshot_observed_at":"2026-07-12T17:50:38.884440Z","submitted_at":"2026-05-02T17:06:26Z","title":"Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron Colliders","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-09T14:19:51.378483Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2605.01539"},"observation_digest":"sha256:124519bb7ea8c654ae649d51e88f008d28c033c186afd8b08c9499e141c99910","observation_id":"eba67638-d1f1-4eaa-93c0-972d6966bc56","resolution":{"observed_at":"2026-05-11T17:01:07.914394Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2605.01921","last_updated":"2026-05-03T15:03:18Z","snapshot_observed_at":"2026-08-07T09:23:46.424550Z","submitted_at":"2026-05-03T15:03:18Z","title":"Hunting for $B\\bar B$ molecular state $X_{b0}$ via radiative transition of $\\Upsilon(10753)$","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-09T16:29:58.668036Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2605.01921"},"observation_digest":"sha256:c602a41f814f7c5c999b18cdf9da15c48098e507c063ddd57389d3d68d8e897a","observation_id":"dbd9cc9d-c9a9-439a-9e11-e9b014cd42a1","resolution":{"observed_at":"2026-05-11T16:31:07.661349Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2605.03320","last_updated":"2026-05-05T03:11:23Z","snapshot_observed_at":"2026-07-06T23:16:15.509235Z","submitted_at":"2026-05-05T03:11:23Z","title":"Does $\\psi(4660)$ exist?","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-05-07T16:16:31.719942Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2605.03320"},"observation_digest":"sha256:fad3a18c3209664231bf5da360f6993e3a2016a7d10b3169fa40fabea6760c51","observation_id":"e071cbf4-44a9-4f23-be1a-d450afda7742","resolution":{"observed_at":"2026-05-12T10:51:31.232641Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2605.26658","last_updated":"2026-05-26T07:43:44Z","snapshot_observed_at":"2026-07-06T23:36:29.930024Z","submitted_at":"2026-05-26T07:43:44Z","title":"Isospin-breaking effects on the threshold cusp structures in $\\Lambda N$-$\\Sigma N$ scattering","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-06-29T17:32:20.687145Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2605.26658"},"observation_digest":"sha256:3885ff508f66d475db1ab19111f3503d998c19e51fc2ac3e47438492326ce6ee","observation_id":"cc99e28d-6da8-4d51-a993-990397f6abc2","resolution":{"observed_at":"2026-06-29T17:33:45.056233Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.06180","last_updated":"2026-06-17T21:06:30Z","snapshot_observed_at":"2026-07-06T23:46:05.829177Z","submitted_at":"2026-06-04T13:53:42Z","title":"Vector charmonium(-like) states in the energy range of 4.1-4.6 GeV","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-06-28T00:42:32.420283Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.06180"},"observation_digest":"sha256:ceed023c96c7046ce0d61659378cc3d8a46651f56e841850905e85f76fcfa20a","observation_id":"daa544e4-a393-4b11-bdc4-f72cbc75299a","resolution":{"observed_at":"2026-07-02T14:07:03.339762Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.07225","last_updated":"2026-06-05T12:42:41Z","snapshot_observed_at":"2026-07-06T23:46:55.970997Z","submitted_at":"2026-06-05T12:42:41Z","title":"Simultaneous Dalitz-plot decomposition of the $e^+ e^- \\to J/\\psi \\, \\pi \\, \\pi \\, (K \\bar{K})$ processes in the 4.13-4.36 GeV region using dispersive final-state interactions","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-06-27T21:54:56.701456Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.07225"},"observation_digest":"sha256:4c2dc2816d1211a40a6a896c9155145e2987f811afc2cf4af688dbb1734201c9","observation_id":"ba8bfe01-b03e-4cd5-b806-24c1c2ec26ba","resolution":{"observed_at":"2026-07-02T17:37:15.073544Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.12309","last_updated":"2026-06-17T13:43:35Z","snapshot_observed_at":"2026-08-04T08:48:17.124755Z","submitted_at":"2026-06-10T16:43:50Z","title":"$\\boldsymbol{\\chi_{c1}}(3872)$ and its Partners in the Diabatic Born-Oppenheimer Approximation for QCD","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-06-27T09:04:17.876386Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.12309"},"observation_digest":"sha256:f336858f2ccb6253b1f7c696d2b038888cdd7bd453d3bbc3c9d53559c3b97320","observation_id":"9ff565c2-1daa-4287-8536-d7355f673df3","resolution":{"observed_at":"2026-07-03T12:18:06.600473Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.24380","last_updated":"2026-06-23T10:11:49Z","snapshot_observed_at":"2026-08-02T16:00:48.292152Z","submitted_at":"2026-06-23T10:11:49Z","title":"Fully-heavy multiquarks in neural-network quantum states","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-06-25T23:46:44.008571Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.24380"},"observation_digest":"sha256:fd6f5f13f481fd4264d2967e3894ef409507cf15be05d3044c46be9ba2c012cb","observation_id":"5a8d105a-6404-4748-b667-33efe932a7cf","resolution":{"observed_at":"2026-07-04T17:20:00.565568Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.24578","last_updated":"2026-06-23T13:42:23Z","snapshot_observed_at":"2026-07-06T23:59:08.580746Z","submitted_at":"2026-06-23T13:42:23Z","title":"First evidence of $X(3872)\\to\\pi^0\\chi_{c0}(1P)$ and search for $X(3915)\\to\\pi^0\\chi_{c1}(1P)$","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-06-25T21:29:19.271205Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.24578"},"observation_digest":"sha256:9dcc0b79fba2945c29c03bcae7ff28ef6fc7fef7c9c9717a18d9620f45c95ce6","observation_id":"d0d7bc24-a02f-4291-a014-4f42be38009a","resolution":{"observed_at":"2026-07-04T19:20:06.766669Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.24764","last_updated":"2026-06-23T16:22:55Z","snapshot_observed_at":"2026-08-01T14:33:08.708055Z","submitted_at":"2026-06-23T16:22:55Z","title":"Radiative decays of dynamically generated pentaquarks in the chiral unitary approach: the $P_c(4457)\\to P_c(4312)\\,\\gamma$ transition","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-06-25T23:19:23.781078Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.24764"},"observation_digest":"sha256:ab1fe941cdf11faf0038a9193aaf0653dc7e9b1e9f3d776ffc2bbc1c69e1221c","observation_id":"bfcf9d72-488f-4724-90b4-9a8166d36fe7","resolution":{"observed_at":"2026-07-04T17:50:01.326425Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":"1907.07583","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-04T19:20:06.764974Z","title":"Brambilla, S","venue":null,"work_id":"8ca0cff2-9579-4577-9985-3ab63d95ae56","year":2020},"citing_paper":{"arxiv_id":"2606.29560","last_updated":"2026-06-28T18:56:11Z","snapshot_observed_at":"2026-08-04T03:35:45.324907Z","submitted_at":"2026-06-28T18:56:11Z","title":"Probing the structure of $\\chi_{c1}(3872)$: Heavy quark symmetries at work","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-06-30T01:55:16.834752Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2606.29560"},"observation_digest":"sha256:b0814659962e8d48ecdc76ab9f456493e32380420ff3e554a72de2722169f11e","observation_id":"aeea6ec5-f305-40ac-8b80-3627dcb0e1e3","resolution":{"observed_at":"2026-06-30T02:54:11.465621Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-02T09:04:00.672234Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.02382","last_updated":"2026-07-30T13:18:44Z","snapshot_observed_at":"2026-08-06T14:51:50.883878Z","submitted_at":"2026-07-02T16:19:35Z","title":"Symmetry Analysis of Compact Tetraquark States and Implications for the Level Ordering of the Fully Charmed Candidates $X(6600)$, $X(6900)$, and $X(7100)$","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-02T09:04:00.672234Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.02382"},"observation_digest":"sha256:f488b477e0f0cd080eb44e210af6495a4eb11bdb4adf6efc1e215d671dc3ea05","observation_id":"f3849cbe-2e82-4c95-ba58-ca55e29a9d21","resolution":{"observed_at":"2026-08-02T09:04:00.672234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-11T15:18:38.162388Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.04679","last_updated":"2026-07-08T19:10:53Z","snapshot_observed_at":"2026-08-06T23:06:01.666934Z","submitted_at":"2026-07-06T05:07:57Z","title":"Possibility of the antibottom-strange molecular pentaquarks near $ B\\Sigma$ and $ B^*\\Sigma$ thresholds","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-07-11T15:18:38.162388Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.04679"},"observation_digest":"sha256:b330d0ab62f792a0459756d46758d7f3580b3308bdb30a2f910c93c21541ace6","observation_id":"72262582-8baa-4fae-82bd-8fabb3b85a77","resolution":{"observed_at":"2026-07-11T15:18:38.162388Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-14T10:23:51.856721Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.10631","last_updated":"2026-07-12T07:47:07Z","snapshot_observed_at":"2026-08-06T05:29:27.959007Z","submitted_at":"2026-07-12T07:47:07Z","title":"$\\lambda$, $\\rho$, and $\\sigma$ Regge trajectories for the quadruply heavy pentaquark $bb\\bar{u}cc$ in the diquark-triquark picture","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-07-14T10:23:51.856721Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.10631"},"observation_digest":"sha256:72ddb0642612e671d44699476154e0f63759edb93acd4661877287c946f56311","observation_id":"93877146-297c-42ff-98d2-ceef3085923a","resolution":{"observed_at":"2026-07-14T10:23:51.856721Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-14T08:58:06.051834Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.10829","last_updated":"2026-07-12T16:44:25Z","snapshot_observed_at":"2026-07-16T23:19:02.366286Z","submitted_at":"2026-07-12T16:44:25Z","title":"A Unified Study of Hidden-Charm and Hidden-Bottom Mesons","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-07-14T08:58:06.051834Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.10829"},"observation_digest":"sha256:6f41dc7525b01b350d570d287584520859a609a7650ea30314c8eefcafc62dbd","observation_id":"e75c54ac-9060-4b1e-b088-9da7625304f7","resolution":{"observed_at":"2026-07-14T08:58:06.051834Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-14T04:55:21.810799Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.11536","last_updated":"2026-07-13T13:19:33Z","snapshot_observed_at":"2026-08-06T06:41:37.910398Z","submitted_at":"2026-07-13T13:19:33Z","title":"An improved moment QCD sum rule","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-07-14T04:55:21.810799Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.11536"},"observation_digest":"sha256:058c72cf293a55fc41b38f2702c65bd1927a24eb419cc7b9cca193bd0e9d6eae","observation_id":"662f995a-1626-4bfd-954c-22dbb16b1230","resolution":{"observed_at":"2026-07-14T04:55:21.810799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-31T11:54:30.566848Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24550","last_updated":"2026-07-27T15:26:20Z","snapshot_observed_at":"2026-08-04T06:03:40.697668Z","submitted_at":"2026-07-27T15:26:20Z","title":"Decay constants of the two-pole $D_0^*(2300)$","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-07-31T11:54:30.566848Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.24550"},"observation_digest":"sha256:b822b9ea68c0def51694d15332b61740ec14ac33eb2961c81d0b1a7dc61a69b1","observation_id":"6b0291d6-0747-4246-8e4b-d266578d79f9","resolution":{"observed_at":"2026-07-31T11:54:30.566848Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-07-31T09:15:13.715061Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.24648","last_updated":"2026-07-27T16:46:35Z","snapshot_observed_at":"2026-08-06T06:46:49.987322Z","submitted_at":"2026-07-27T16:46:35Z","title":"Analytic decomposition of two-body electroweak processes with left-hand cuts","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-07-31T09:15:13.715061Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.24648"},"observation_digest":"sha256:195e0ff06bc80e5b7a2912b3858da6809173e9c57c4b66cc67a31e1e0f0148e4","observation_id":"12c0cfae-de6c-4712-b5a8-d35cba23fd5a","resolution":{"observed_at":"2026-07-31T09:15:13.715061Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-01T02:38:14.155455Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.25401","last_updated":"2026-07-28T08:01:29Z","snapshot_observed_at":"2026-08-06T07:29:03.950700Z","submitted_at":"2026-07-28T08:01:29Z","title":"Singly heavy tetraquarks","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-01T02:38:14.155455Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.25401"},"observation_digest":"sha256:aaf4f6e359866245f220ce55373e480a6ab1359946f7c2b59cd23e5aca44e5bf","observation_id":"d43f1b22-b212-4dba-b32a-f39cbd224a80","resolution":{"observed_at":"2026-08-01T02:38:14.155455Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07583","snapshot_observed_at":"2026-08-01T04:05:26.461157Z","title":"Brambilla, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.27653","last_updated":"2026-07-30T04:06:09Z","snapshot_observed_at":"2026-08-02T23:37:23.345472Z","submitted_at":"2026-07-30T04:06:09Z","title":"Magnetic dipole moments as probes of doubly-bottom molecular pentaquarks","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-01T04:05:26.461157Z"},"links":{"cited_paper":"/paper/1907.07583","citing_paper":"/paper/2607.27653"},"observation_digest":"sha256:c538d0901aa364e588baa07e97a13c38e43fd0f80047fe52322bcd7a5428fa2f","observation_id":"da6ea96e-2dbc-44ce-ab37-d0e5c1c248d4","resolution":{"observed_at":"2026-08-01T04:05:26.461157Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1907.07583/citation-record","integrity":"/paper/1907.07583/integrity","json":"/paper/1907.07583/citation-record.json","paper":"/paper/1907.07583"},"outbound":[],"paper":{"arxiv_id":"1907.07583","last_updated":"2020-05-14T02:25:38Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-04T20:46:36.933380Z","submitted_at":"2019-07-17T15:28:47Z","title":"The $XYZ$ states: experimental and theoretical status and perspectives"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"thesis":"As of 7 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 59 inbound Pith citation observations for arXiv:1907.07583."}