2,788 research outputs found
Author Correction: A portrait of the Higgs boson by the CMS experiment ten years after the discovery
No full textIn the version of this article initially published, CMS Collaboration author names, affiliations and acknowledgements were omitted and have now been included in the HTML and PDF versions of the articl
Author Correction: A portrait of the Higgs boson by the CMS experiment ten years after the discovery (Nature, (2022), 607, 7917, (60-68), 10.1038/s41586-022-04892-x)
No full textCorrection to: Nature Published online 4 July 2022 In the version of this article initially published, CMS Collaboration author names, affiliations and acknowledgements were omitted and have now been included in the HTML and PDF versions of the article.0info:eu-repo/semantics/publishe
Acceleration and isobaric separation of radioactive ion beams with the Louvain-la-Neuve isochronous cyclotrons
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Author Correction: A portrait of the Higgs boson by the CMS experiment ten years after the discovery
No full textCorrection to: Nature Published online 4 July 2022 In the version of this article initially published, CMS Collaboration author names, affiliations and acknowledgements were omitted and have now been included in the HTML and PDF versions of the article
Author Correction: A portrait of the Higgs boson by the CMS experiment ten years after the discovery (Nature, (2022), 607, 7917, (60-68), 10.1038/s41586-022-04892-x)
No full textCorrection to: Nature Published online 4 July 2022 In the version of this article initially published, CMS Collaboration author names, affiliations and acknowledgements were omitted and have now been included in the HTML and PDF versions of the article.SCOAP
Search for a heavy composite Majorana neutrino in events with dilepton signatures from proton-proton collisions at √s=13 Tev
No full textResults are presented of a search for a heavy Majorana neutrino N ⠃ decaying into two same-flavor leptons ⠃ (electrons or muons) and a quark-pair jet. A model is considered in which the N ⠃ is an excited neutrino in a compositeness scenario. The analysis is performed using a sample of proton-proton collisions at & RADIC;s = 13 TeV recorded by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 138 fb-1. The data are found to be in agreement with the standard model prediction. For the process in which the N ⠃ is produced in association with a lepton, followed by the decay of the N ⠃ to a same-flavor lepton and a quark pair, an upper limit at 95% confidence level on the product of the cross section and branching fraction is obtained as a function of the N ⠃ mass mN ⠃ and the compositeness scale ⠄. For this model the data exclude the existence of Ne (N & mu;) for mN ⠃ below 6.0 (6.1) TeV, at the limit where mN ⠃ is equal to ⠄. For mN ⠃ N 1 TeV, values of ⠄ less than 20 (23) TeV are excluded. These results represent a considerable improvement in sensitivity, covering a larger parameter space than previous searches in pp collisions at 13 TeV.& COPY; 2023 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons .org /licenses /by /4 .0/). Funded by SCOAP3
Acceleration and mass-separation of radioactive ion beams in an isochronous cyclotron
No full textThe authors report on first operational results obtained with the two-cyclotron concept for the production and acceleration of a /sup 13 /N radioactive beam (/b T//sub 1/2/=10 min.). A pure beam of 70 particle pA of /sup 13/N at 0.63 meV/amu has been accelerated and used for cross-section measurements of the /sup 1/H(/sup 13 /N, gamma )/sup 14/O reaction which is involved in astrophysical processes. Although the /sup 13/N beam is accelerated with a /sup 13/C beam at least 10/sup 3/ times more intense, the specific characteristics of a cyclotron make it possible to separate clearly these two species whose relative mass difference is only 1.8*10/sup -4/, without loss of intensity for the /sup 13 /N beam. The /sup 13/C contamination on the final target is less than 1 particle pA. The advantages of a cyclotron over a linac as a post-accelerator for low-energy radioactive beams are discussed.Anglai
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