Cargando…
Physics with ions at the Future Circular Collider
The unique physics opportunities accessible with nuclear collisions at the CERN Future Circular Collider (FCC) are summarized. Lead-lead (PbPb) and proton-lead (pPb) collisions at sNN=39 and 63 TeV respectively with Lint=33nb−1 and 8 pb −1 monthly integrated luminosities, will provide unprecedented...
Autores principales: | , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2017
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nuclphysa.2017.06.029 http://cds.cern.ch/record/2263136 |
_version_ | 1780954167981899776 |
---|---|
author | d'Enterria, David Apolinario, L. Armesto, N. Dainese, A. Jowett, J. Lansberg, J.P. Masciocchi, S. Milhano, G. Roland, C. Salgado, C.A. Schaumann, M. van Leeuwen, M. Wiedemann, U.A. |
author_facet | d'Enterria, David Apolinario, L. Armesto, N. Dainese, A. Jowett, J. Lansberg, J.P. Masciocchi, S. Milhano, G. Roland, C. Salgado, C.A. Schaumann, M. van Leeuwen, M. Wiedemann, U.A. |
author_sort | d'Enterria, David |
collection | CERN |
description | The unique physics opportunities accessible with nuclear collisions at the CERN Future Circular Collider (FCC) are summarized. Lead-lead (PbPb) and proton-lead (pPb) collisions at sNN=39 and 63 TeV respectively with Lint=33nb−1 and 8 pb −1 monthly integrated luminosities, will provide unprecedented experimental conditions to study quark-gluon matter at temperatures O(1 GeV). The following topics are succinctly discussed: (i) charm-quark densities thrice larger than at the LHC, leading to direct heavy-quark impact in the bulk QGP properties, (ii) quarkonia, including ϒ(1S) , melting at temperatures up to five times above the QCD critical temperature, (iii) access to initial-state nuclear parton distributions (nPDF) at fractional momenta as low as x≈10−7 , (iv) availability of about 5⋅105 top-quark pairs per run to study the high- x gluon nPDF and the energy loss properties of boosted colour-antennas, (v) study of possible Higgs boson suppression in the QGP, and (vi) high-luminosity γγ (ultraperipheral) collisions at c.m. energies up to 1 TeV. |
id | cern-2263136 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2017 |
record_format | invenio |
spelling | cern-22631362023-03-14T19:33:36Zdoi:10.1016/j.nuclphysa.2017.06.029http://cds.cern.ch/record/2263136engd'Enterria, DavidApolinario, L.Armesto, N.Dainese, A.Jowett, J.Lansberg, J.P.Masciocchi, S.Milhano, G.Roland, C.Salgado, C.A.Schaumann, M.van Leeuwen, M.Wiedemann, U.A.Physics with ions at the Future Circular Collidernucl-thNuclear Physics - Theorynucl-exNuclear Physics - Experimenthep-phParticle Physics - Phenomenologyhep-exParticle Physics - ExperimentThe unique physics opportunities accessible with nuclear collisions at the CERN Future Circular Collider (FCC) are summarized. Lead-lead (PbPb) and proton-lead (pPb) collisions at sNN=39 and 63 TeV respectively with Lint=33nb−1 and 8 pb −1 monthly integrated luminosities, will provide unprecedented experimental conditions to study quark-gluon matter at temperatures O(1 GeV). The following topics are succinctly discussed: (i) charm-quark densities thrice larger than at the LHC, leading to direct heavy-quark impact in the bulk QGP properties, (ii) quarkonia, including ϒ(1S) , melting at temperatures up to five times above the QCD critical temperature, (iii) access to initial-state nuclear parton distributions (nPDF) at fractional momenta as low as x≈10−7 , (iv) availability of about 5⋅105 top-quark pairs per run to study the high- x gluon nPDF and the energy loss properties of boosted colour-antennas, (v) study of possible Higgs boson suppression in the QGP, and (vi) high-luminosity γγ (ultraperipheral) collisions at c.m. energies up to 1 TeV.The unique physics opportunities accessible with nuclear collisions at the CERN Future Circular Collider (FCC) are summarized. Lead-lead (PbPb) and proton-lead (pPb) collisions at $\sqrt{s_{NN}}$ = 39 and 63 TeV respectively with $\mathcal{L}_{int}$ = 33 nb$^{-1}$ and 8 pb$^{-1}$ monthly integrated luminosities, will provide unprecedented experimental conditions to study quark-gluon matter at temperatures ${\cal O}$(1 GeV). The following topics are succinctly discussed: (i) charm-quark densities thrice larger than at the LHC, leading to direct heavy-quark impact in the bulk QGP properties, (ii) quarkonia, including $\Upsilon(1S)$, melting at temperatures up to five times above the QCD critical temperature, (iii) access to initial-state nuclear parton distributions (nPDF) at fractional momenta as low as $x\approx 10^{-7}$, (iv) availability of $5\cdot 10^5$ top-quark pairs per run to study the high-$x$ gluon nPDF and the energy loss properties of boosted colour-antennas, (v) study of possible Higgs boson suppression in the QGP, and (vi) high-luminosity $\gamma\gamma$ (ultraperipheral) collisions at c.m. energies up to 1 TeV.arXiv:1704.05891oai:cds.cern.ch:22631362017-04-19 |
spellingShingle | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment d'Enterria, David Apolinario, L. Armesto, N. Dainese, A. Jowett, J. Lansberg, J.P. Masciocchi, S. Milhano, G. Roland, C. Salgado, C.A. Schaumann, M. van Leeuwen, M. Wiedemann, U.A. Physics with ions at the Future Circular Collider |
title | Physics with ions at the Future Circular Collider |
title_full | Physics with ions at the Future Circular Collider |
title_fullStr | Physics with ions at the Future Circular Collider |
title_full_unstemmed | Physics with ions at the Future Circular Collider |
title_short | Physics with ions at the Future Circular Collider |
title_sort | physics with ions at the future circular collider |
topic | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment |
url | https://dx.doi.org/10.1016/j.nuclphysa.2017.06.029 http://cds.cern.ch/record/2263136 |
work_keys_str_mv | AT denterriadavid physicswithionsatthefuturecircularcollider AT apolinariol physicswithionsatthefuturecircularcollider AT armeston physicswithionsatthefuturecircularcollider AT dainesea physicswithionsatthefuturecircularcollider AT jowettj physicswithionsatthefuturecircularcollider AT lansbergjp physicswithionsatthefuturecircularcollider AT masciocchis physicswithionsatthefuturecircularcollider AT milhanog physicswithionsatthefuturecircularcollider AT rolandc physicswithionsatthefuturecircularcollider AT salgadoca physicswithionsatthefuturecircularcollider AT schaumannm physicswithionsatthefuturecircularcollider AT vanleeuwenm physicswithionsatthefuturecircularcollider AT wiedemannua physicswithionsatthefuturecircularcollider |