{"as_of":"2026-08-15T12:31:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:419fd066261d2fd38a706e8f0f02d92d07ed023de9fb75d7157a9c7f2b587996","coverage":[{"denominator":61,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":61,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T10:10:20.401768Z","state":"measured"},{"denominator":61,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":61,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-15T06:32:42.880941+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1909.00013/citation-record","integrity":"/paper/1909.00013/integrity","json":"/paper/1909.00013/citation-record.json","paper":"/paper/1909.00013"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.578583Z","title":null,"venue":null,"work_id":"9107be75-190d-4694-880a-ac6edf2926dc","year":null},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.088786Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:226c0f85b179173b2c1806ea531473c9a23604121f480f389e541802fa8c0282","observation_id":"0c31abd0-b04d-44bf-a4c7-89d627674be3","resolution":{"observed_at":"2026-08-14T10:10:21.584261Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.562470Z","title":"In the ﬁrst case, we can determine all coeﬃcients us- ing the continuity of A and the ﬁrst three derivatives at the point Q2 = Q2 P to ﬁx all the coeﬃcients","venue":null,"work_id":"1a9283d5-8c86-41d1-80b2-5e2d4f6d5e89","year":2007},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.094808Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:4227317cf8a6984e000efd38b6488f59ac4cca40d672bd111370a407bcfba6a6","observation_id":"5761c497-6e60-4ed3-8a5d-b22a62b4e0f9","resolution":{"observed_at":"2026-08-14T10:10:21.568251Z","resolver_source":"raw_fallback","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.547473Z","title":null,"venue":null,"work_id":"358215da-af18-432b-baf5-2ed0d9ff1e59","year":null},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.100976Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:89b98d95161744574aa56613f7878a78c1cf7797a3801211779cff5aafae6d40","observation_id":"001a0674-3e8f-44fa-b9dd-58373177a1c1","resolution":{"observed_at":"2026-08-14T10:10:21.552491Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.532716Z","title":"The coeﬃcient α3 can then be de- termined by Eq","venue":null,"work_id":"06ff64b6-87c8-435f-afbf-a0d8eba66bf0","year":null},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.106223Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:536a80e714d47a61446324093d2cefe506b4001189d2e287664f3bad737056ae","observation_id":"be84442d-275a-4053-932c-52c91161d882","resolution":{"observed_at":"2026-08-14T10:10:21.537614Z","resolver_source":"raw_fallback","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1212.4891","last_updated":"2013-04-03T18:23:16Z","snapshot_observed_at":"2026-08-15T00:35:03.541857Z","submitted_at":"2012-12-20T00:44:03Z","title":"Studies of Nucleon Resonance Structure in Exclusive Meson Electroproduction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.4891","snapshot_observed_at":"2026-08-14T10:10:20.111598Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.111598Z"},"links":{"cited_paper":"/paper/1212.4891","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:9e8b519aea0a8228abcf7e62bf026a20f608420224f4cc69745fc747c788d3da","observation_id":"6ec5a1dc-aab0-49c8-af41-fcbafa8ebc41","resolution":{"observed_at":"2026-08-14T10:10:20.111598Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.08587","last_updated":"2018-08-10T18:07:21Z","snapshot_observed_at":"2026-08-14T20:45:04.998521Z","submitted_at":"2017-07-26T18:01:27Z","title":"Polarization Transfer Observables in Elastic Electron Proton Scattering at $Q^2 = $2.5, 5.2, 6.8, and 8.5 GeV$^2$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.08587","snapshot_observed_at":"2026-08-14T10:10:20.117075Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.117075Z"},"links":{"cited_paper":"/paper/1707.08587","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:cc5268117e32428306ca3b0f33af6692f7f1ca04caaf537b842832b76cf08f68","observation_id":"bd248cc1-a1f1-4d1c-8040-6663e82bb50f","resolution":{"observed_at":"2026-08-14T10:10:20.117075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.1720","last_updated":"2011-11-16T08:28:08Z","snapshot_observed_at":"2026-08-15T11:00:27.221412Z","submitted_at":"2011-09-07T14:51:34Z","title":"Electroexcitation of nucleon resonances","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.1720","snapshot_observed_at":"2026-08-14T10:10:20.122689Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.122689Z"},"links":{"cited_paper":"/paper/1109.1720","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:2895d0b6b2e708c712c449aa26270dbd104ecb1c791dd7906b161a7c576ff09d","observation_id":"a3c92d28-2a28-431f-980e-31201c902346","resolution":{"observed_at":"2026-08-14T10:10:20.122689Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0710.0306","last_updated":"2007-10-01T14:19:39Z","snapshot_observed_at":"2026-08-15T10:31:10.543555Z","submitted_at":"2007-10-01T14:19:39Z","title":"Unitary Isobar Model - MAID2007","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0710.0306","snapshot_observed_at":"2026-08-14T10:10:20.127792Z","title":"Drechsel, S","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.127792Z"},"links":{"cited_paper":"/paper/0710.0306","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:e5ac106dd8a0ca4f81a4497fadb09a8e9578b3f18198ca297d1d2b44066d3f77","observation_id":"56ecd2af-78df-4b51-a25a-c0daf7656554","resolution":{"observed_at":"2026-08-14T10:10:20.127792Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.1723","last_updated":"2009-04-24T21:50:41Z","snapshot_observed_at":"2026-08-15T05:53:16.974406Z","submitted_at":"2009-03-10T09:57:15Z","title":"The Nucleon Distribution Amplitudes and their application to nucleon form factors and the $N \\to \\Delta$ transition at intermediate values of $Q^2$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.1723","snapshot_observed_at":"2026-08-14T10:10:20.133534Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.133534Z"},"links":{"cited_paper":"/paper/0903.1723","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:a03814a9b475ceffce6e620c897b66c276f5c27f541d65942fffcd526fe0dd62","observation_id":"69fc5c81-888e-47a5-b9c9-cfdacc735424","resolution":{"observed_at":"2026-08-14T10:10:20.133534Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0905.1944","last_updated":"2009-05-20T00:51:03Z","snapshot_observed_at":"2026-08-15T05:48:35.369001Z","submitted_at":"2009-05-12T19:47:02Z","title":"N to $\\Delta$ transition amplitudes from QCD sum rules","version":2},"cited_work":{"arxiv_id":"0905.1944","doi":null,"metadata_source":"pith","pith_arxiv_id":"0905.1944","snapshot_observed_at":"2026-08-14T10:10:21.205289Z","title":"N to $\\Delta$ transition amplitudes from QCD sum rules","venue":"hep-ph","work_id":"57fb7f23-c6cf-4704-b92e-facd7c7e7155","year":2009},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.139404Z"},"links":{"cited_paper":"/paper/0905.1944","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:de0c0145c877208c6203b837e95ad81ff60498a7b8665eb92cd72931ad63d32b","observation_id":"29df7bd8-1234-40ac-9667-47bf0cd3738d","resolution":{"observed_at":"2026-08-14T10:10:21.210429Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1505.05759","last_updated":"2015-05-26T12:07:59Z","snapshot_observed_at":"2026-08-14T22:47:38.727428Z","submitted_at":"2015-05-21T14:55:59Z","title":"Electroproduction of the $N^\\ast(1535)$ nucleon resonance in QCD","version":2},"cited_work":{"arxiv_id":"1505.05759","doi":null,"metadata_source":"pith","pith_arxiv_id":"1505.05759","snapshot_observed_at":"2026-08-14T10:10:21.182922Z","title":"Electroproduction of the $N^\\ast(1535)$ nucleon resonance in QCD","venue":"hep-ph","work_id":"0156fb2a-26ee-48b3-a4d8-c3a8c80d9a2d","year":2015},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.144848Z"},"links":{"cited_paper":"/paper/1505.05759","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:9e3539beac288968343c626523ad05430eb7061ece41d3db028db57ce73b7bde","observation_id":"0a14e38c-535f-42bc-9f46-d00f78fba709","resolution":{"observed_at":"2026-08-14T10:10:21.188128Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.09602","last_updated":"2016-07-22T16:31:50Z","snapshot_observed_at":"2026-08-14T21:50:22.108150Z","submitted_at":"2016-06-30T18:16:12Z","title":"Baryons as relativistic three-quark bound states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.09602","snapshot_observed_at":"2026-08-14T10:10:20.150105Z","title":"Eichmann, H","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.150105Z"},"links":{"cited_paper":"/paper/1606.09602","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:40d9dfe68b54e73e643574ba2da1c5090d95429f7f17044dd0786b1c17200e80","observation_id":"4c663887-4d6f-4cef-ba86-5d5d3f3c239a","resolution":{"observed_at":"2026-08-14T10:10:20.150105Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.04405","last_updated":"2016-07-15T07:36:21Z","snapshot_observed_at":"2026-08-14T21:48:16.872154Z","submitted_at":"2016-07-15T07:36:21Z","title":"Dissecting nucleon transition electromagnetic form factors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.04405","snapshot_observed_at":"2026-08-14T10:10:20.155152Z","title":"Segovia and C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.155152Z"},"links":{"cited_paper":"/paper/1607.04405","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:afd91f66e46a6d2d09ee668a10de0485afb90c7be7c506059022395cc8347b0f","observation_id":"abc01e8b-05aa-4422-a7c2-b12f9543932c","resolution":{"observed_at":"2026-08-14T10:10:20.155152Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.0965","last_updated":"2011-08-04T00:30:22Z","snapshot_observed_at":"2026-08-15T04:39:06.665258Z","submitted_at":"2011-08-04T00:30:22Z","title":"Excited Baryons in Holographic QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.0965","snapshot_observed_at":"2026-08-14T10:10:20.160372Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.160372Z"},"links":{"cited_paper":"/paper/1108.0965","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:12def5b5d198276d31f14c57ea7c6c603c674b140a6d5c092fc776f3ca558b52","observation_id":"7a879288-ca6d-4e0b-a134-0ac59c553f4f","resolution":{"observed_at":"2026-08-14T10:10:20.160372Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.8131","last_updated":"2015-02-13T18:20:52Z","snapshot_observed_at":"2026-08-14T23:24:50.103686Z","submitted_at":"2014-07-30T17:23:56Z","title":"Light-Front Holographic QCD and Emerging Confinement","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.8131","snapshot_observed_at":"2026-08-14T10:10:20.165531Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.165531Z"},"links":{"cited_paper":"/paper/1407.8131","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:f399adf7a8b936b85e76dffc6058e0b40342172c6e86bb07df08b6d1e8818ea1","observation_id":"28bebd5d-030f-4b88-8944-b8aae0942c64","resolution":{"observed_at":"2026-08-14T10:10:20.165531Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.6020","last_updated":"2012-11-13T17:32:00Z","snapshot_observed_at":"2026-08-15T00:45:14.775225Z","submitted_at":"2012-09-26T18:02:06Z","title":"Production of negative parity baryons in the holographic Sakai-Sugimoto model","version":3},"cited_work":{"arxiv_id":"1209.6020","doi":null,"metadata_source":"pith","pith_arxiv_id":"1209.6020","snapshot_observed_at":"2026-08-14T10:10:21.091313Z","title":"Production of negative parity baryons in the holographic Sakai-Sugimoto model","venue":"hep-ph","work_id":"a36f3e2e-f9f4-4ebd-a199-668230b13a10","year":2012},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.170670Z"},"links":{"cited_paper":"/paper/1209.6020","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:75062d9b0565b4320709a2e60a36bbd73c5df67531e17b687612656c694c0cb0","observation_id":"d30cb508-0933-4aee-9c09-c1901092eda6","resolution":{"observed_at":"2026-08-14T10:10:21.096843Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1703.03819","last_updated":"2018-03-03T17:16:27Z","snapshot_observed_at":"2026-08-14T21:12:26.028149Z","submitted_at":"2017-03-10T19:01:58Z","title":"Valence quark contributions for the $\\gamma^\\ast N \\to N(1440)$ form factors from Light-Front holography","version":2},"cited_work":{"arxiv_id":"1703.03819","doi":null,"metadata_source":"pith","pith_arxiv_id":"1703.03819","snapshot_observed_at":"2026-08-14T10:10:21.069156Z","title":"Valence quark contributions for the $\\gamma^\\ast N \\to N(1440)$ form factors from Light-Front holography","venue":"hep-ph","work_id":"6eeac2d2-516b-4896-a290-f1cc85362d21","year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.175356Z"},"links":{"cited_paper":"/paper/1703.03819","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:2e1058b82edd69b9365524e9c23086aa2b2b37732a098cbb3bfa7e33d1660f6e","observation_id":"c0c91d94-f158-492f-be69-982145fc03dc","resolution":{"observed_at":"2026-08-14T10:10:21.074547Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1712.08410","last_updated":"2017-12-25T14:02:31Z","snapshot_observed_at":"2026-08-14T20:00:51.898237Z","submitted_at":"2017-12-22T11:57:44Z","title":"Electromagnetic structure of nucleon and Roper in soft-wall AdS/QCD","version":2},"cited_work":{"arxiv_id":"1712.08410","doi":null,"metadata_source":"pith","pith_arxiv_id":"1712.08410","snapshot_observed_at":"2026-08-14T10:10:21.047418Z","title":"Electromagnetic structure of nucleon and Roper in soft-wall AdS/QCD","venue":"hep-ph","work_id":"05c6c110-faa7-4caf-b84a-c6d62368f7fb","year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.180262Z"},"links":{"cited_paper":"/paper/1712.08410","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:a816e0f80007649f569cb9c50e8ffdfc1fad2c0b1132ecfac5fa19427abfa103","observation_id":"5a1f7486-43b8-4ed7-8489-059672f0f3fe","resolution":{"observed_at":"2026-08-14T10:10:21.052613Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1306.3864","last_updated":"2014-01-27T18:04:26Z","snapshot_observed_at":"2026-08-15T00:13:50.637588Z","submitted_at":"2013-06-17T14:02:27Z","title":"Electromagnetic structure of the nucleon and the Roper resonance in a light-front quark approach","version":2},"cited_work":{"arxiv_id":"1306.3864","doi":null,"metadata_source":"pith","pith_arxiv_id":"1306.3864","snapshot_observed_at":"2026-08-14T10:10:21.023706Z","title":"Electromagnetic structure of the nucleon and the Roper resonance in a light-front quark approach","venue":"hep-ph","work_id":"bf0d9169-1777-4923-b2e1-f7cb6435017d","year":2013},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.185114Z"},"links":{"cited_paper":"/paper/1306.3864","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b25f9d4f599610206f5485a9b907239d3fb9eb1ce745fbc3c526cdb09d09eaf9","observation_id":"5e3468d6-1bad-48ba-ad02-7eeb55eece5e","resolution":{"observed_at":"2026-08-14T10:10:21.029476Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1201.5759","last_updated":"2012-01-27T12:22:45Z","snapshot_observed_at":"2026-08-15T09:55:13.888617Z","submitted_at":"2012-01-27T12:22:45Z","title":"Nucleon electromagnetic form factors and electroexcitation of low lying nucleon resonances in a light-front relativistic quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.5759","snapshot_observed_at":"2026-08-14T10:10:20.190089Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.190089Z"},"links":{"cited_paper":"/paper/1201.5759","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:837401821c792a88cedba37bff6f999f7cffcc286ff097ef425fb74a328938f8","observation_id":"699e9a76-b6a7-4722-b9ed-24af4aef9387","resolution":{"observed_at":"2026-08-14T10:10:20.190089Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.01207","last_updated":"2015-06-03T11:07:10Z","snapshot_observed_at":"2026-08-14T22:45:57.685943Z","submitted_at":"2015-06-03T11:07:10Z","title":"A systematic study of longitudinal and transverse helicity amplidutes in the hypercentral Constituent Quark Model","version":1},"cited_work":{"arxiv_id":"1506.01207","doi":null,"metadata_source":"pith","pith_arxiv_id":"1506.01207","snapshot_observed_at":"2026-08-14T10:10:20.983797Z","title":"A systematic study of longitudinal and transverse helicity amplidutes in the hypercentral Constituent Quark Model","venue":"nucl-th","work_id":"76d0593b-adc8-4691-bda0-60a28287eddf","year":2015},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.194997Z"},"links":{"cited_paper":"/paper/1506.01207","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:d5b414774d4ea245cf6cc7005886debc4dbefe2461d21f5e0341cf0e5a9cb6e7","observation_id":"a24b9416-fe50-4a2b-9caa-9e47c8d6665c","resolution":{"observed_at":"2026-08-14T10:10:20.990138Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1105.2484","last_updated":"2011-08-15T15:39:16Z","snapshot_observed_at":"2026-08-15T04:46:59.641373Z","submitted_at":"2011-05-12T14:25:05Z","title":"A simple relation between the gamma N -> N(1535) helicity amplitudes","version":2},"cited_work":{"arxiv_id":"1105.2484","doi":null,"metadata_source":"pith","pith_arxiv_id":"1105.2484","snapshot_observed_at":"2026-08-14T10:10:20.960700Z","title":"A simple relation between the gamma N -> N(1535) helicity amplitudes","venue":"hep-ph","work_id":"2d3be7ed-58cb-4dd1-be46-b59a6b81dad7","year":2011},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.199630Z"},"links":{"cited_paper":"/paper/1105.2484","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b108bb34bcb0cedfe53f5b723d5d6a9c09e1a5aeb17873bd887066c49791de72","observation_id":"f912216c-fa5a-4f3f-81b5-53f8775f1bdc","resolution":{"observed_at":"2026-08-14T10:10:20.966413Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1407.0649","last_updated":"2014-08-15T18:26:11Z","snapshot_observed_at":"2026-08-14T23:28:11.722627Z","submitted_at":"2014-07-02T17:01:04Z","title":"Using the Single Quark Transition Model to predict nucleon resonance amplitudes","version":2},"cited_work":{"arxiv_id":"1407.0649","doi":null,"metadata_source":"pith","pith_arxiv_id":"1407.0649","snapshot_observed_at":"2026-08-14T10:10:20.937657Z","title":"Using the Single Quark Transition Model to predict nucleon resonance amplitudes","venue":"hep-ph","work_id":"fc1bccb7-e821-4e52-9d4a-e5cd6002a8fc","year":2014},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.204185Z"},"links":{"cited_paper":"/paper/1407.0649","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b56a6110ee0bd5a43b0256b20af912d9209c624df35fc6007cab83395fce9855","observation_id":"bce4630d-0c5e-4cae-a68f-ace2857a1b98","resolution":{"observed_at":"2026-08-14T10:10:20.943283Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9904072","last_updated":"1999-04-28T10:15:26Z","snapshot_observed_at":"2026-07-07T06:41:57.907727Z","submitted_at":"1999-04-28T10:15:26Z","title":"Pion cloud and the $Q^2-$dependence of $\\gamma^* N \\leftrightarrow \\Delta$ transition form factors","version":1},"cited_work":{"arxiv_id":"nucl-th/9904072","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/9904072","snapshot_observed_at":"2026-08-14T10:10:20.912325Z","title":"Pion cloud and the $Q^2-$dependence of $\\gamma^* N \\leftrightarrow \\Delta$ transition form factors","venue":"nucl-th","work_id":"92b7ca9e-d23d-4244-8a25-1f7f639768c7","year":1999},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.209393Z"},"links":{"cited_paper":"/paper/nucl-th/9904072","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:41b5c9febe4ed06e8fe8a6a986962acc87be6ca69e3cead716e5b1d656997886","observation_id":"7528c086-1128-4a54-9e17-93c96b361a10","resolution":{"observed_at":"2026-08-14T10:10:20.918264Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0407020","last_updated":"2004-07-21T23:20:07Z","snapshot_observed_at":"2026-08-03T03:15:49.242889Z","submitted_at":"2004-07-21T23:20:07Z","title":"Electromagnetic Meson Production in the Nucleon Resonance Region","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0407020","snapshot_observed_at":"2026-08-14T10:10:20.214301Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.214301Z"},"links":{"cited_paper":"/paper/nucl-ex/0407020","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:6ea53565832d2c3e8583da3d86732eeb623317f6ba17759b8e0458c84891fafc","observation_id":"c0ff9083-0bbd-405d-abd1-afdcacff1ee8","resolution":{"observed_at":"2026-08-14T10:10:20.214301Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0611033","last_updated":"2006-12-15T04:04:29Z","snapshot_observed_at":"2026-08-15T10:57:20.689330Z","submitted_at":"2006-11-09T22:51:29Z","title":"Extraction and Interpretation of gamma N --> Delta Form Factors within a Dynamical Model","version":2},"cited_work":{"arxiv_id":"nucl-th/0611033","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/0611033","snapshot_observed_at":"2026-08-14T10:10:20.870570Z","title":"Extraction and Interpretation of gamma N --> Delta Form Factors within a Dynamical Model","venue":"nucl-th","work_id":"2a2500c9-1e5c-4de3-b943-16e07d84db47","year":2006},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.219935Z"},"links":{"cited_paper":"/paper/nucl-th/0611033","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:71a1b036205cac40dc37733b50c9a254df85208cbb79e68e5594b7e2a7556e20","observation_id":"fdd8de1f-4a8b-43ac-b51e-301a76ba7c57","resolution":{"observed_at":"2026-08-14T10:10:20.876164Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.517869Z","title":null,"venue":null,"work_id":"61cb074a-45f3-42e3-b537-0d338fc33190","year":1966},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.225103Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:a1fcf25236a7afaa8d27e27c16bde78a704328a3571ef90efe492bd634691cbe","observation_id":"0bfb8d35-b2e6-4692-885e-cffd8d8794b6","resolution":{"observed_at":"2026-08-14T10:10:21.522362Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.502259Z","title":null,"venue":null,"work_id":"8e9b8c2b-a52e-4b4b-a2f3-36d0ca009b59","year":1973},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.229962Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:41c1c47dc2b8a714f340ef01f525d6648236d94c21b0cd0aaf5ca2e6d598ff7c","observation_id":"13833188-7206-4b9c-a83e-2e64bce20b55","resolution":{"observed_at":"2026-08-14T10:10:21.507682Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.487480Z","title":null,"venue":null,"work_id":"8679c8aa-ffa0-4440-82de-7f7b1709a46c","year":1976},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.234676Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:d4de11f79b0268b676e4ff3094afc332b81abd442c06edb5ab3d493d35aa9a38","observation_id":"e64302f6-f16d-4ae1-805e-cafe662a3cc3","resolution":{"observed_at":"2026-08-14T10:10:21.492206Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1806.04579","last_updated":"2018-06-12T15:03:02Z","snapshot_observed_at":"2026-08-14T19:04:41.742037Z","submitted_at":"2018-06-12T15:03:02Z","title":"Nucleon resonances in Compton scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.04579","snapshot_observed_at":"2026-08-14T10:10:20.239319Z","title":"Eichmann and G","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.239319Z"},"links":{"cited_paper":"/paper/1806.04579","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:2a85394adf800a0b90a68439c1a7de692cb7a19bbcfcdce4cd1c6f4f4a7f62b9","observation_id":"48abb802-2080-4ce5-aff3-c43b4bfa7324","resolution":{"observed_at":"2026-08-14T10:10:20.239319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.03444","last_updated":"2016-05-27T01:41:12Z","snapshot_observed_at":"2026-08-14T22:10:52.656385Z","submitted_at":"2016-02-10T16:57:41Z","title":"Improved empirical parametrizations of the $\\gamma^\\ast N \\to N(1535)$ transition amplitudes and the Siegert's theorem","version":2},"cited_work":{"arxiv_id":"1602.03444","doi":null,"metadata_source":"pith","pith_arxiv_id":"1602.03444","snapshot_observed_at":"2026-08-14T10:10:20.830957Z","title":"Improved empirical parametrizations of the $\\gamma^\\ast N \\to N(1535)$ transition amplitudes and the Siegert's theorem","venue":"hep-ph","work_id":"56953e4d-2081-45bf-ab0d-15b5545480b1","year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.244412Z"},"links":{"cited_paper":"/paper/1602.03444","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:561e184eb1f9ce8f8782050b7b11e311fabc61d531e0a52e3fd803422476a71f","observation_id":"9c0bb55a-f43e-4aa7-ab6c-9cb701b578c0","resolution":{"observed_at":"2026-08-14T10:10:20.836251Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1602.03832","last_updated":"2016-05-30T20:45:37Z","snapshot_observed_at":"2026-08-15T11:30:55.388250Z","submitted_at":"2016-02-11T19:18:42Z","title":"Improved empirical parametrizations of the $\\gamma^\\ast N \\to \\Delta(1232)$ and $\\gamma^\\ast N \\to N(1520)$ helicity amplitudes and the Siegert's theorem","version":2},"cited_work":{"arxiv_id":"1602.03832","doi":null,"metadata_source":"pith","pith_arxiv_id":"1602.03832","snapshot_observed_at":"2026-08-14T10:10:20.807635Z","title":"Improved empirical parametrizations of the $\\gamma^\\ast N \\to \\Delta(1232)$ and $\\gamma^\\ast N \\to N(1520)$ helicity amplitudes and the Siegert's theorem","venue":"hep-ph","work_id":"7f72bb53-9a2b-4868-8c0b-d8fe460a3e2c","year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.250403Z"},"links":{"cited_paper":"/paper/1602.03832","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:f9149e9ba615e2d2dc0157d59015cfcee3d9d1a339398e24d329022029503ad4","observation_id":"77f24bb3-ef19-431f-b15d-7ca96ac4ea63","resolution":{"observed_at":"2026-08-14T10:10:20.813550Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1904.08016","last_updated":"2019-04-16T23:30:41Z","snapshot_observed_at":"2026-08-15T09:11:15.440138Z","submitted_at":"2019-04-16T23:30:41Z","title":"Nucleon resonance contributions to unpolarised inclusive electron scattering","version":1},"cited_work":{"arxiv_id":"1904.08016","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.08016","snapshot_observed_at":"2026-08-14T10:10:20.784407Z","title":"Nucleon resonance contributions to unpolarised inclusive electron scattering","venue":"hep-ph","work_id":"ec6c454c-4af8-4928-abb7-01224657d92c","year":2019},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.255240Z"},"links":{"cited_paper":"/paper/1904.08016","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:9f883f445cb61fb9523ecd2e142f34e2f9b5b52b389dc2a93388f73e2d117cfb","observation_id":"6bceb15b-5246-4fce-9117-d5e91183586a","resolution":{"observed_at":"2026-08-14T10:10:20.789452Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.471811Z","title":"Drechsel and L","venue":null,"work_id":"3566ea01-ed65-4a7d-9b38-3bbe4252a9a6","year":1992},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.260397Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:08e1fe36297e63c65881c4a6c6af07152fdb93ab08861c79a8cf3bc74e9a3666","observation_id":"7f172419-b333-47ee-bf0f-1b50e6a04826","resolution":{"observed_at":"2026-08-14T10:10:21.476626Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.454618Z","title":"Amaldi, S","venue":null,"work_id":"7d2fe66f-800c-4780-a26b-be4b0c0a2cfe","year":1979},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.265102Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:ad9a7859c814821499217ef45e8a711c3d3261d55e479d6540a6f53b83a5507a","observation_id":"3e0dcba0-538e-4ede-8b27-0ed749b964d8","resolution":{"observed_at":"2026-08-14T10:10:21.459791Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.439326Z","title":"Tiator, Few Body Syst","venue":null,"work_id":"7385070d-25be-44d3-9bfb-89176cd85d8f","year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.270745Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:2aa36f0d112650a1cad3713f343a5242c6cad7bdaf647f22423bb0df85d18ebe","observation_id":"5205881d-4d9e-41c7-9244-d61816fa8a05","resolution":{"observed_at":"2026-08-14T10:10:21.443975Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.423435Z","title":null,"venue":null,"work_id":"07b24eda-6802-438d-b8cd-66e1922633ad","year":null},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.275484Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:0fb805461d88d0364c51ed22a70a45ca3eac71920422290ceb3d7ac50b9945dd","observation_id":"5e53ebe3-10b3-4ac3-9480-266e76d830d2","resolution":{"observed_at":"2026-08-14T10:10:21.428250Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.408573Z","title":null,"venue":null,"work_id":"8278fcea-0545-478a-b1d2-c7ac84939dfd","year":null},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.280230Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:d8c56942e0f6b5b2fc87f717131b977fc4c7bb196c467bab372029c28b521f48","observation_id":"10c7dfa9-a205-472f-bad8-d0785bc0a62f","resolution":{"observed_at":"2026-08-14T10:10:21.413196Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0909.2349","last_updated":"2009-09-16T06:20:28Z","snapshot_observed_at":"2026-08-15T05:39:14.651750Z","submitted_at":"2009-09-12T16:05:37Z","title":"Electroexcitation of nucleon resonances from CLAS data on single pion electroproduction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.2349","snapshot_observed_at":"2026-08-14T10:10:20.285039Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.285039Z"},"links":{"cited_paper":"/paper/0909.2349","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:f1f5bef1219f8dd899c7eab276b0d4a7ba77980318814c8af2746545c36fc36b","observation_id":"c4ae8d17-2618-4143-98dc-95a7999bb8a5","resolution":{"observed_at":"2026-08-14T10:10:20.285039Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1205.3948","last_updated":"2012-07-20T15:22:00Z","snapshot_observed_at":"2026-08-15T00:59:46.678529Z","submitted_at":"2012-05-17T14:58:38Z","title":"A study of the $P_{11}(1440)$ and $D_{13}(1520)$ resonances from CLAS data on $ep \\rightarrow e'\\pi^{+} \\pi^{-} p'$","version":3},"cited_work":{"arxiv_id":"1205.3948","doi":null,"metadata_source":"pith","pith_arxiv_id":"1205.3948","snapshot_observed_at":"2026-08-14T10:10:20.747254Z","title":"A study of the $P_{11}(1440)$ and $D_{13}(1520)$ resonances from CLAS data on $ep \\rightarrow e'\\pi^{+} \\pi^{-} p'$","venue":"nucl-ex","work_id":"4e62c92e-8ec1-4aba-bf9d-537c61b0b783","year":2012},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.290414Z"},"links":{"cited_paper":"/paper/1205.3948","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:c0e4181888b6232614d6b81e31efebe91ab04b080264eb75eaefd22de553b03f","observation_id":"405e9f9a-e2a9-4c84-b140-83512a84d30d","resolution":{"observed_at":"2026-08-14T10:10:20.752213Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1509.05460","last_updated":"2015-12-15T14:22:06Z","snapshot_observed_at":"2026-08-14T22:31:53.296524Z","submitted_at":"2015-09-17T22:14:52Z","title":"New Results from the Studies of the $N(1440)1/2^+$, $N(1520)3/2^-$, and $\\Delta(1620)1/2^-$ Resonances in Exclusive $ep \\to e'p' \\pi^+ \\pi^-$ Electroproduction with the CLAS Detector","version":3},"cited_work":{"arxiv_id":"1509.05460","doi":null,"metadata_source":"pith","pith_arxiv_id":"1509.05460","snapshot_observed_at":"2026-08-14T10:10:20.726283Z","title":"New Results from the Studies of the $N(1440)1/2^+$, $N(1520)3/2^-$, and $\\Delta(1620)1/2^-$ Resonances in Exclusive $ep \\to e'p' \\pi^+ \\pi^-$ Electroproduction with the CLAS Detector","venue":"nucl-ex","work_id":"ca69959b-e967-4911-b34e-c06c80f01077","year":2015},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.295527Z"},"links":{"cited_paper":"/paper/1509.05460","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:d45da1f0a829368fdffb7381c18ab2f73d7b93b8b64fbdbef4d0dfc65c5e4da3","observation_id":"78d30f00-db19-48de-85b3-b81ba42994cb","resolution":{"observed_at":"2026-08-14T10:10:20.731675Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.392950Z","title":null,"venue":null,"work_id":"36147639-be69-444a-8c90-d961d9f891c6","year":1998},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.300615Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:e09f448a8415f51251be339cfa56100fabd4b445bf7af60d8de55f4b17f8d775","observation_id":"c71cd25a-a367-430d-bb09-52ebfd341d7c","resolution":{"observed_at":"2026-08-14T10:10:21.397834Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1002.3386","last_updated":"2010-04-20T17:05:45Z","snapshot_observed_at":"2026-08-15T05:26:21.329855Z","submitted_at":"2010-02-17T21:36:36Z","title":"Valence quark contributions for the gamma N -> P11(1440) form factors","version":3},"cited_work":{"arxiv_id":"1002.3386","doi":null,"metadata_source":"pith","pith_arxiv_id":"1002.3386","snapshot_observed_at":"2026-08-14T10:10:20.705260Z","title":"Valence quark contributions for the gamma N -> P11(1440) form factors","venue":"hep-ph","work_id":"73e64390-6922-4d3b-94fa-2a3b129e59ef","year":2010},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.305442Z"},"links":{"cited_paper":"/paper/1002.3386","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:164ad5d861f2d906e25af2cee15c1c1a8625a9c1937ae9d8ab28b73d9b6de5a5","observation_id":"30bba05a-2fee-4e35-a609-f06875b01c2d","resolution":{"observed_at":"2026-08-14T10:10:20.710317Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.03042","last_updated":"2016-12-10T22:20:09Z","snapshot_observed_at":"2026-08-15T10:23:00.924023Z","submitted_at":"2016-06-09T18:06:42Z","title":"Parametrizations of the $\\gamma^\\ast N \\to \\Delta(1232)$ quadrupole form factors and Siegert's theorem","version":2},"cited_work":{"arxiv_id":"1606.03042","doi":null,"metadata_source":"pith","pith_arxiv_id":"1606.03042","snapshot_observed_at":"2026-08-14T10:10:20.682498Z","title":"Parametrizations of the $\\gamma^\\ast N \\to \\Delta(1232)$ quadrupole form factors and Siegert's theorem","venue":"hep-ph","work_id":"2e8a777c-6079-49e0-a2d4-b7e5d0ee9f40","year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.310620Z"},"links":{"cited_paper":"/paper/1606.03042","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:f2ae57b6e7a5035656298364cd55e1b21925694e32544dd1731b8f187f065135","observation_id":"23bf1114-b70f-40b8-90c6-a15af3f03420","resolution":{"observed_at":"2026-08-14T10:10:20.688381Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1709.07412","last_updated":"2018-05-17T21:20:29Z","snapshot_observed_at":"2026-08-14T20:30:56.380900Z","submitted_at":"2017-09-21T16:56:47Z","title":"New low-$Q^2$ measurements of the $\\gamma^\\ast N \\to \\Delta(1232)$ Coulomb quadrupole form factor, pion cloud parametrizations and Siegert's theorem","version":2},"cited_work":{"arxiv_id":"1709.07412","doi":null,"metadata_source":"pith","pith_arxiv_id":"1709.07412","snapshot_observed_at":"2026-08-14T10:10:20.660344Z","title":"New low-$Q^2$ measurements of the $\\gamma^\\ast N \\to \\Delta(1232)$ Coulomb quadrupole form factor, pion cloud parametrizations and Siegert's theorem","venue":"hep-ph","work_id":"05174cd8-e961-4c77-8b74-d688bbfc1c4b","year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.315706Z"},"links":{"cited_paper":"/paper/1709.07412","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b1ecba97fc6851f8b6530476b7c16e48a047650c377987f38834088374391f93","observation_id":"cbdb763d-7828-4a68-8d42-d36eaf308793","resolution":{"observed_at":"2026-08-14T10:10:20.665843Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1710.10527","last_updated":"2019-03-07T19:02:37Z","snapshot_observed_at":"2026-08-14T20:19:19.914883Z","submitted_at":"2017-10-28T20:29:50Z","title":"Combined parametrization of the neutron electric form factor and the $\\gamma^\\ast N \\to \\Delta(1232)$ quadrupole form factors","version":2},"cited_work":{"arxiv_id":"1710.10527","doi":null,"metadata_source":"pith","pith_arxiv_id":"1710.10527","snapshot_observed_at":"2026-08-14T10:10:20.635979Z","title":"Combined parametrization of the neutron electric form factor and the $\\gamma^\\ast N \\to \\Delta(1232)$ quadrupole form factors","venue":"hep-ph","work_id":"3aa2efce-cbe9-4e1d-bb18-c4a44040e649","year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.321704Z"},"links":{"cited_paper":"/paper/1710.10527","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:4abe8e96600baf72182dad25f6990a45294c7f7059862e8c3b54449b1ddc55ff","observation_id":"ad2e19be-24a5-4ed1-8fc0-9f10aefa58af","resolution":{"observed_at":"2026-08-14T10:10:20.642866Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9610040","last_updated":"1996-10-25T13:16:24Z","snapshot_observed_at":"2026-08-11T18:26:01.677029Z","submitted_at":"1996-10-25T13:16:24Z","title":"Electromagnetic Properties of the Delta(1232)","version":1},"cited_work":{"arxiv_id":"nucl-th/9610040","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/9610040","snapshot_observed_at":"2026-08-14T10:10:20.611469Z","title":"Electromagnetic Properties of the Delta(1232)","venue":"nucl-th","work_id":"e6e4973b-7e6c-4a13-b76c-1b19f8a01a87","year":1996},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.326872Z"},"links":{"cited_paper":"/paper/nucl-th/9610040","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b2e54f9162de4ae3bb14487e5fa0766676f36a9b7974f3066fe66c2466a6eee0","observation_id":"4eaddb98-d5c9-4d01-b626-2507d60fd06d","resolution":{"observed_at":"2026-08-14T10:10:20.616867Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0412421","last_updated":"2004-12-30T17:19:21Z","snapshot_observed_at":"2026-07-07T04:06:17.361609Z","submitted_at":"2004-12-30T17:19:21Z","title":"Electromagnetic N->Delta transition and neutron form factors","version":1},"cited_work":{"arxiv_id":"hep-ph/0412421","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0412421","snapshot_observed_at":"2026-08-14T10:10:20.588353Z","title":"Electromagnetic N->Delta transition and neutron form factors","venue":"hep-ph","work_id":"c7336904-62ff-4bfe-a055-97fa0a7937a6","year":2004},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.331730Z"},"links":{"cited_paper":"/paper/hep-ph/0412421","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:9de8ecc69eddcaa1b5425953a090671562e76a37012c764c5fca12fb76153ee3","observation_id":"9e033394-d9f1-450f-8dd6-567af4e1506a","resolution":{"observed_at":"2026-08-14T10:10:20.593544Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:20.336674Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.336674Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:e078356c0afa26092889ac5c1f9ee332681ed69afe82d2c6f4e835be10f01e43","observation_id":"fe9ed1a3-ac5d-499a-963d-d2aece145a7e","resolution":{"observed_at":"2026-08-14T10:10:20.336674Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.366457Z","title":"Stajner et al","venue":null,"work_id":"52ee122a-93b1-45c0-8e4c-578b4e100efd","year":2017},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.341894Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:ffe22777878758ed213b69ffdde3985ece8fe7bc4e09a6c2f477ba6eceabd894","observation_id":"12f0dbeb-ca0a-49f1-a3d9-e1e2ebf23de9","resolution":{"observed_at":"2026-08-14T10:10:21.371310Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1412.0274","last_updated":"2014-12-17T21:38:37Z","snapshot_observed_at":"2026-08-14T23:09:36.721949Z","submitted_at":"2014-11-30T20:07:15Z","title":"Measurements of $ep \\to e^\\prime \\pi^+n$ at W = 1.6 - 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS","version":3},"cited_work":{"arxiv_id":"1412.0274","doi":null,"metadata_source":"pith","pith_arxiv_id":"1412.0274","snapshot_observed_at":"2026-08-14T10:10:20.565174Z","title":"Measurements of $ep \\to e^\\prime \\pi^+n$ at W = 1.6 - 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS","venue":"nucl-ex","work_id":"f3defbce-b9f0-42a1-8b34-199991022f78","year":2014},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.347116Z"},"links":{"cited_paper":"/paper/1412.0274","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b4c8f98bb7db38234e4d3bbb7b08f16029491e18a299cd943e288566a6a8489b","observation_id":"e197f13e-5bce-47c5-b413-18beb1837c41","resolution":{"observed_at":"2026-08-14T10:10:20.570472Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1310.1101","last_updated":"2013-10-03T20:07:14Z","snapshot_observed_at":"2026-08-15T00:00:27.796934Z","submitted_at":"2013-10-03T20:07:14Z","title":"Studies of N^* structure from the CLAS meson electroproduction data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.1101","snapshot_observed_at":"2026-08-14T10:10:20.352496Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.352496Z"},"links":{"cited_paper":"/paper/1310.1101","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:8ed3bf8ad87e058f25cc0c4f164bcc1a470c89414a22b36fc8b2e4915c495e93","observation_id":"1ff12798-6245-424e-8c2f-6e0523286fe5","resolution":{"observed_at":"2026-08-14T10:10:20.352496Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.350690Z","title":"Blomberg et al","venue":null,"work_id":"2afbf955-358e-4bcc-a3a4-d373cdd161f9","year":2016},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.360803Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:134918d705fb53adb09309c2be2e81319b5bd8fed57ccf6fc02dc7db3bbe06e5","observation_id":"2811788e-97dc-4318-be73-84215c636b2d","resolution":{"observed_at":"2026-08-14T10:10:21.355856Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.333782Z","title":"Stave et al","venue":null,"work_id":"ade1c4a8-7cf7-4b77-894e-a6a3d25b8f1b","year":2008},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.366667Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:3e7ae2eb823368088110e26226731f49caa729d1c0d334032a2f4db78862d997","observation_id":"71d782db-5ee0-4cc9-916f-8b331abac0b6","resolution":{"observed_at":"2026-08-14T10:10:21.339457Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.318179Z","title":"Sparveris et al","venue":null,"work_id":"d9420cbe-d3e2-4fdf-be1f-827206f7c71d","year":2013},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.371761Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:c47aec6bca3fcbf2fd92a4a27a128229c28db853b029229c5cbc72eb4d2d96b5","observation_id":"3145ad01-815d-4883-ad4b-866dfa6412b9","resolution":{"observed_at":"2026-08-14T10:10:21.322865Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1508.04088","last_updated":"2015-08-17T17:17:40Z","snapshot_observed_at":"2026-08-14T22:36:16.164402Z","submitted_at":"2015-08-17T17:17:40Z","title":"Recent results on the nucleon resonance spectrum and structure from the CLAS detector","version":1},"cited_work":{"arxiv_id":"1508.04088","doi":null,"metadata_source":"pith","pith_arxiv_id":"1508.04088","snapshot_observed_at":"2026-08-14T10:10:20.524638Z","title":"Recent results on the nucleon resonance spectrum and structure from the CLAS detector","venue":"nucl-ex","work_id":"b837293f-bea8-49de-b1f4-d70011f8be09","year":2015},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.376826Z"},"links":{"cited_paper":"/paper/1508.04088","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:a4fbc458a381005bb880167470f20672620591852ce4c505d8ca9eb343c518b8","observation_id":"808be667-7759-4204-af65-38b538a0f20c","resolution":{"observed_at":"2026-08-14T10:10:20.531211Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0903.1110","last_updated":"2009-05-05T18:11:40Z","snapshot_observed_at":"2026-08-15T05:53:32.196805Z","submitted_at":"2009-03-05T22:00:50Z","title":"$\\pi^+$ photoproduction on the proton for photon energies from 0.725 to 2.875 GeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.1110","snapshot_observed_at":"2026-08-14T10:10:20.382024Z","title":"Dugger et al","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.382024Z"},"links":{"cited_paper":"/paper/0903.1110","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:cb3681049ec441145f7eaada9d04460fb2a5dd23cbc2b25c0d8ce87912ea42e2","observation_id":"787f0af7-5149-4def-95a0-906f5cdd12fa","resolution":{"observed_at":"2026-08-14T10:10:20.382024Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.3034","last_updated":"2008-03-20T17:09:46Z","snapshot_observed_at":"2026-08-15T10:21:13.002710Z","submitted_at":"2008-03-20T17:09:46Z","title":"A Covariant model for the nucleon and the $\\Delta$","version":1},"cited_work":{"arxiv_id":"0803.3034","doi":null,"metadata_source":"pith","pith_arxiv_id":"0803.3034","snapshot_observed_at":"2026-08-14T10:10:20.484330Z","title":"A Covariant model for the nucleon and the $\\Delta$","venue":"hep-ph","work_id":"cee145f1-5307-4477-9a4b-50124e1bcd10","year":2008},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.387111Z"},"links":{"cited_paper":"/paper/0803.3034","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:8535d359c876ace5c9bee2139986888672fb2fac057cccd62684a7e6f04ede88","observation_id":"f5be30d8-2394-40b1-a548-990fbb79c1f2","resolution":{"observed_at":"2026-08-14T10:10:20.490482Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0901.4310","last_updated":"2009-07-10T21:21:10Z","snapshot_observed_at":"2026-08-15T12:17:03.548752Z","submitted_at":"2009-01-27T18:55:37Z","title":"Valence quark contribution for the gamma N -> Delta quadrupole transition extracted from lattice QCD","version":2},"cited_work":{"arxiv_id":"0901.4310","doi":null,"metadata_source":"pith","pith_arxiv_id":"0901.4310","snapshot_observed_at":"2026-08-14T10:10:20.457747Z","title":"Valence quark contribution for the gamma N -> Delta quadrupole transition extracted from lattice QCD","venue":"hep-ph","work_id":"d75de6d6-11f8-4001-8431-1a9d9624021f","year":2009},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.392015Z"},"links":{"cited_paper":"/paper/0901.4310","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:6d3f5853217eb9802363ad4edaf971ba6363c0941bb6a89c4242496d1be46028","observation_id":"1536defd-d541-4822-b184-5ee7863ed4a1","resolution":{"observed_at":"2026-08-14T10:10:20.465013Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T10:10:21.301832Z","title":null,"venue":null,"work_id":"e81cdd1f-36ea-4565-a13b-ae48eaf898d6","year":2005},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.397117Z"},"links":{"citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:b777bcc860796efb71c6cf651c9208c231b841513ac64a82090cb6bb87fd7a40","observation_id":"51d720c0-7f57-46ff-983f-8bfa676e81a7","resolution":{"observed_at":"2026-08-14T10:10:21.307014Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0609004","last_updated":"2006-10-06T07:53:33Z","snapshot_observed_at":"2026-07-07T04:12:07.006377Z","submitted_at":"2006-09-01T06:04:27Z","title":"Electromagnetic excitation of the Delta(1232)-resonance","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0609004","snapshot_observed_at":"2026-08-14T10:10:20.401768Z","title":"Pascalutsa, M","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T10:10:20.401768Z"},"links":{"cited_paper":"/paper/hep-ph/0609004","citing_paper":"/paper/1909.00013"},"observation_digest":"sha256:cb2fb82d0ed5c0d88d040aae8f0700b82038b4b6c859dcc01982d1f8c4609be7","observation_id":"e34d305e-c530-4ab0-acd0-45c75e255e17","resolution":{"observed_at":"2026-08-14T10:10:20.401768Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1909.00013","last_updated":"2019-12-11T19:08:42Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-15T09:11:03.840319Z","submitted_at":"2019-08-30T18:02:25Z","title":"Low-$Q^2$ empirical parametrizations of the $N^\\ast$ helicity amplitudes"},"reference_resolution":{"displayed":61,"state_counts":{"malformed_identifier":2,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":26,"verified_exact":26,"verified_fuzzy":7},"total_outbound_references":61},"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":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 61 of 61 outbound references and 0 inbound Pith citation observations for arXiv:1909.00013."}