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Atracci\u00f3n Talento, CM, Spain"},{"name":"SRC, Sweden"}],"content-domain":{"domain":["journals.aps.org"],"crossmark-restriction":true},"short-container-title":["Phys. Rev. Lett."],"accepted":{"date-parts":[[2026,6,9]]},"abstract":"\n The first observation of the doubly charmed baryon\n \n \n \u039e<\/a:mi>\n \n c<\/a:mi>\n c<\/a:mi>\n <\/a:mrow>\n +<\/a:mo>\n <\/a:msubsup>\n <\/a:math>\n is reported through its decay to the\n \n \n \n \n \u039b<\/d:mi>\n <\/d:mrow>\n \n c<\/d:mi>\n <\/d:mrow>\n \n +<\/d:mo>\n <\/d:mrow>\n <\/d:msubsup>\n \n \n K<\/d:mi>\n <\/d:mrow>\n \n \u2212<\/d:mo>\n <\/d:mrow>\n <\/d:msup>\n \n \n \u03c0<\/d:mi>\n <\/d:mrow>\n \n +<\/d:mo>\n <\/d:mrow>\n <\/d:msup>\n <\/d:mrow>\n <\/d:math>\n final state, with a statistical significance exceeding seven standard deviations. The observation is made using proton-proton collision data collected in 2024 with the LHCb Run 3 detector at a center-of-mass energy of 13.6\u00a0TeV, corresponding to a total integrated luminosity of\n \n 6.9<\/g:mn>\n \u2009<\/g:mtext>\n \u2009<\/g:mtext>\n \n fb<\/g:mi>\n \n \u2212<\/g:mo>\n 1<\/g:mn>\n <\/g:mrow>\n <\/g:msup>\n <\/g:math>\n . The\n \n \n \u039e<\/i:mi>\n \n c<\/i:mi>\n c<\/i:mi>\n <\/i:mrow>\n +<\/i:mo>\n <\/i:msubsup>\n <\/i:math>\n mass is measured to be\n \n \n 3619.97<\/l:mn>\n \u00b1<\/l:mo>\n 0.83<\/l:mn>\n \u00b1<\/l:mo>\n \n \n 0.26<\/l:mn>\n <\/l:mrow>\n \n \u2212<\/l:mo>\n 1.30<\/l:mn>\n <\/l:mrow>\n \n +<\/l:mo>\n 1.90<\/l:mn>\n <\/l:mrow>\n <\/l:msubsup>\n \u2009<\/l:mtext>\n \u2009<\/l:mtext>\n \n MeV<\/l:mi>\n \/<\/l:mo>\n \n \n c<\/l:mi>\n <\/l:mrow>\n \n 2<\/l:mn>\n <\/l:mrow>\n <\/l:msup>\n <\/l:mrow>\n <\/l:mrow>\n <\/l:math>\n , where the first uncertainty is statistical, the second is systematic, and the third is due to the unknown\n \n \n \u039e<\/n:mi>\n \n c<\/n:mi>\n c<\/n:mi>\n <\/n:mrow>\n +<\/n:mo>\n <\/n:msubsup>\n <\/n:math>\n lifetime, which is assumed to lie in the range 15\u2013160\u00a0fs with a baseline value of 45\u00a0fs. The difference between the masses of the\n \n \n \u039e<\/q:mi>\n \n c<\/q:mi>\n c<\/q:mi>\n <\/q:mrow>\n +<\/q:mo>\n <\/q:msubsup>\n <\/q:math>\n and\n \n \n \u039e<\/t:mi>\n \n c<\/t:mi>\n c<\/t:mi>\n <\/t:mrow>\n \n +<\/t:mo>\n +<\/t:mo>\n <\/t:mrow>\n <\/t:msubsup>\n <\/t:math>\n baryons is determined to be\n \n \n \u2212<\/w:mo>\n 1.77<\/w:mn>\n \u00b1<\/w:mo>\n 0.84<\/w:mn>\n \u00b1<\/w:mo>\n \n \n 0.15<\/w:mn>\n <\/w:mrow>\n \n \u2212<\/w:mo>\n 1.30<\/w:mn>\n <\/w:mrow>\n \n +<\/w:mo>\n 1.90<\/w:mn>\n <\/w:mrow>\n <\/w:msubsup>\n \u2009<\/w:mtext>\n \u2009<\/w:mtext>\n MeV<\/w:mi>\n \/<\/w:mo>\n \n \n c<\/w:mi>\n <\/w:mrow>\n \n 2<\/w:mn>\n <\/w:mrow>\n <\/w:msup>\n <\/w:mrow>\n <\/w:math>\n . This is the first observation of a new particle made with the LHCb Run 3 detector.\n <\/jats:p>","DOI":"10.1103\/dmv6-7gdv","type":"journal-article","created":{"date-parts":[[2026,6,9]],"date-time":"2026-06-09T18:12:48Z","timestamp":1781028768000},"update-policy":"https:\/\/doi.org\/10.1103\/crossmark-policy","source":"Crossref","is-referenced-by-count":3,"title":["Observation of the Doubly Charmed Baryon\n \n \n \n \n \u039e<\/mml:mi>\n <\/mml:mrow>\n \n c<\/mml:mi>\n c<\/mml:mi>\n <\/mml:mrow>\n \n +<\/mml:mo>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:mrow>\n <\/mml:math>\n with the LHCb Run 3 Detector"],"prefix":"10.1103","volume":"137","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-0533-1952","authenticated-orcid":true,"given":"R.","family":"Aaij","sequence":"first","affiliation":[{"name":"Nikhef National Institute for Subatomic 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