European Physical Journal C: Particles and Fields (May 2019)
Nuclear dependence of light neutral meson production in p–A collisions at 400 GeV with NA60
- R. Arnaldi,
- K. Banicz,
- K. Borer,
- J. Castor,
- B. Chaurand,
- W. Chen,
- C. Cicalò,
- A. Colla,
- P. Cortese,
- S. Damjanovic,
- A. David,
- A. De Falco,
- A. Devaux,
- L. Ducroux,
- H. En’yo,
- J. Fargeix,
- A. Ferretti,
- M. Floris,
- A. Förster,
- P. Force,
- N. Guettet,
- A. Guichard,
- H. Gulkanian,
- J. M. Heuser,
- P. Jarron,
- M. Keil,
- L. Kluberg,
- Z. Li,
- C. Lourenço,
- J. Lozano,
- F. Manso,
- P. Martins,
- A. Masoni,
- A. Neves,
- H. Ohnishi,
- C. Oppedisano,
- P. Parracho,
- P. Pillot,
- T. Poghosyan,
- G. Puddu,
- E. Radermacher,
- P. Ramalhete,
- P. Rosinsky,
- E. Scomparin,
- J. Seixas,
- S. Serci,
- R. Shahoyan,
- P. Sonderegger,
- H. J. Specht,
- R. Tieulent,
- A. Uras,
- G. Usai,
- R. Veenhof,
- H. K. Wöhri,
- NA60 Collaboration
Affiliations
- R. Arnaldi
- INFN
- K. Banicz
- CERN
- K. Borer
- University of Bern
- J. Castor
- LPC, Université Clermont Auvergne and CNRS-IN2P3
- B. Chaurand
- LLR, Ecole Polytechnique and CNRS-IN2P3
- W. Chen
- BNL, Upton
- C. Cicalò
- INFN
- A. Colla
- INFN
- P. Cortese
- Università di Torino
- S. Damjanovic
- CERN
- A. David
- CERN
- A. De Falco
- INFN
- A. Devaux
- LPC, Université Clermont Auvergne and CNRS-IN2P3
- L. Ducroux
- IPN-Lyon, Univ. Claude Bernard Lyon-I and CNRS-IN2P3
- H. En’yo
- University of Bern
- J. Fargeix
- LPC, Université Clermont Auvergne and CNRS-IN2P3
- A. Ferretti
- INFN
- M. Floris
- INFN
- A. Förster
- CERN
- P. Force
- LPC, Université Clermont Auvergne and CNRS-IN2P3
- N. Guettet
- CERN
- A. Guichard
- IPN-Lyon, Univ. Claude Bernard Lyon-I and CNRS-IN2P3
- H. Gulkanian
- YerPhI
- J. M. Heuser
- RIKEN, Wako
- P. Jarron
- CERN
- M. Keil
- CERN
- L. Kluberg
- LLR, Ecole Polytechnique and CNRS-IN2P3
- Z. Li
- BNL, Upton
- C. Lourenço
- CERN
- J. Lozano
- Instituto Superior Tecnico, Dep. Fisica
- F. Manso
- LPC, Université Clermont Auvergne and CNRS-IN2P3
- P. Martins
- CERN
- A. Masoni
- INFN
- A. Neves
- Instituto Superior Tecnico, Dep. Fisica
- H. Ohnishi
- RIKEN, Wako
- C. Oppedisano
- INFN
- P. Parracho
- CERN
- P. Pillot
- IPN-Lyon, Univ. Claude Bernard Lyon-I and CNRS-IN2P3
- T. Poghosyan
- YerPhI
- G. Puddu
- Università di Cagliari
- E. Radermacher
- CERN
- P. Ramalhete
- CERN
- P. Rosinsky
- CERN
- E. Scomparin
- INFN
- J. Seixas
- Instituto Superior Tecnico, Dep. Fisica
- S. Serci
- INFN
- R. Shahoyan
- CERN
- P. Sonderegger
- Instituto Superior Tecnico, Dep. Fisica
- H. J. Specht
- Physikalisches Institut der Universität Heidelberg
- R. Tieulent
- IPN-Lyon, Univ. Claude Bernard Lyon-I and CNRS-IN2P3
- A. Uras
- INFN
- G. Usai
- INFN
- R. Veenhof
- Instituto Superior Tecnico, Dep. Fisica
- H. K. Wöhri
- CERN
- NA60 Collaboration
- DOI
- https://doi.org/10.1140/epjc/s10052-019-6848-7
- Journal volume & issue
-
Vol. 79,
no. 5
pp. 1 – 13
Abstract
Abstract The NA60 experiment has studied low-mass muon pair production in proton–nucleus collisions with a system of Be, Cu, In, W, Pb and U targets, using a 400 GeV proton beam at the CERN SPS. The transverse momentum spectra of the $$\rho /\omega $$ ρ/ω and $$\phi $$ ϕ mesons are measured in the full $$p_{\mathrm {T}}$$ pT range accessible, from $$p_{\mathrm {T}}= 0$$ pT=0 up to $$2 \, {\hbox {GeV/c}}$$ 2GeV/c . The nuclear dependence of the production cross sections of the $$\eta $$ η , $$\omega $$ ω and $$\phi $$ ϕ mesons has been found to be consistent with the power law $$\sigma _{\mathrm {pA}} \propto {\mathrm {A}}^\alpha $$ σpA∝Aα , with the $$\alpha $$ α parameter increasing as a function of $$p_{\mathrm {T}}$$ pT for all the particles, and an approximate hierarchy $$\alpha _\eta \approx \alpha _\phi > \alpha _\omega $$ αη≈αϕ>αω . The cross section ratios $$\sigma _\eta /\sigma _\omega $$ ση/σω , $$\sigma _\rho /\sigma _\omega $$ σρ/σω and $$\sigma _\phi /\sigma _\omega $$ σϕ/σω have been studied as a function of the size A of the production target, and an increase of the $$\eta $$ η and $$\phi $$ ϕ yields relative to the $$\omega $$ ω is observed from p–Be to p–U collisions.