NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.A.Salgado Found 59 matches. 2019AP02 Nucl.Phys. A982, 795c (2019) L.Apolinario, G.Milhano, C.A.Salgado, G.Salam Unveiling the yoctosecond structure of the QGP with top quarks
doi: 10.1016/j.nuclphysa.2018.11.014
2018AP02 Phys.Rev.Lett. 120, 232301 (2018) L.Apolinario, J.Guilherme Milhano, G.P.Salam, C.A.Salgado Probing the Time Structure of the Quark-Gluon Plasma with Top Quarks
doi: 10.1103/PhysRevLett.120.232301
2017AN14 Nucl.Phys. A967, 492 (2017) C.Andres, N.Armesto, H.Niemi, R.Paatelainen, C.A.Salgado, P.Zurita Extracting q-hat in event-by-event hydrodynamics and the centrality/energy puzzle
doi: 10.1016/j.nuclphysa.2017.05.115
2017CA26 Nucl.Phys. A967, 564 (2017) J.Casalderrey-Solana, Y.Mehtar-Tani, C.A.Salgado, K.Tywoniuk Probing jet decoherence in heavy ion collisions
doi: 10.1016/j.nuclphysa.2017.07.008
2016AP02 Nucl.Phys. A956, 681 (2016) L.Apolinario, N.Armesto, G.Milhano, C.A.Salgado In-medium jet evolution: interplay between broadening and decoherence effects: The XXVth International Conference on Ultrarelativistic Nucleus-Nucleus Collisions
doi: 10.1016/j.nuclphysa.2016.02.043
2016AR07 Nucl.Phys. A956, 525 (2016) N.Armesto, H.Paukkunen, J.M.Penin, C.A.Salgado, P.Zurita Re-weighting at the LHC: the p-Pb data impact
doi: 10.1016/j.nuclphysa.2016.04.026
2016AR08 Nucl.Phys. A956, 854 (2016) N.Armesto, A.Dainese, D.d'Enterria, S.Masciocchi, C.Roland, C.A.Salgado, M.van Leeuwen, U.A.Wiedemann Nuclear collisions at the Future Circular Collider
doi: 10.1016/j.nuclphysa.2016.02.051
2015AN13 Phys.Rev. C 92, 034901 (2015) C.Andres, J.Dias de Deus, A.Moscoso, C.Pajares, C.A.Salgado Universal geometrical scaling of the elliptic flow
doi: 10.1103/PhysRevC.92.034901
2014AP01 Nucl.Phys. A932, 152c (2014) L.Apolinario, N.Armesto, G.Milhano, C.A.Salgado Medium-induced gluon radiation beyond the eikonal approximation
doi: 10.1016/j.nuclphysa.2014.07.032
2014CA38 Nucl.Phys. A932, 269c (2014) M.R.Calvo, M.R.Moldes, C.A.Salgado Radiation spectrum of a massive quark-gluon antenna
doi: 10.1016/j.nuclphysa.2014.10.016
2013AR06 Nucl.Phys. 910-911, 363c (2013) N.Armesto, H.Ma, M.Martinez, Y.Mehtar-Tani, C.A.Salgado Coherence and broadening effects in medium induced gluon radiation
doi: 10.1016/j.nuclphysa.2012.12.058
2013HE14 Nucl.Phys. A904-905, 999c (2013) I.Helenius, K.J.Eskola, H.Honkanen, C.A.Salgado EPS09s and EKS98s: Impact parameter dependent nPDF sets
doi: 10.1016/j.nuclphysa.2013.02.183
2013HE23 Nucl.Phys. 910-911, 510c (2013) I.Helenius, K.J.Eskola, H.Honkanen, C.A.Salgado Modeling the Impact Parameter Dependence of the nPDFs With EKS98 and EPS09 Global Fits
doi: 10.1016/j.nuclphysa.2012.12.040
2013PA18 Phys.Rev.Lett. 110, 212301 (2013) Agreement of Neutrino Deep Inelastic Scattering Data with Global Fits of Parton Distributions
doi: 10.1103/PhysRevLett.110.212301
2013SA47 Nucl.Phys. 910-911, 185c (2013) Theory summary. Hard Probes 2012
doi: 10.1016/j.nuclphysa.2012.12.087
2012AR11 Phys.Rev. C 86, 064904 (2012) N.Armesto, B.Cole, C.Gale, W.A.Horowitz, P.Jacobs, S.Jeon, M.van Leeuwen, A.Majumder, B.Muller, G.-Y.Qin, C.A.Salgado, B.Schenke, M.Verweij, X.-N.Wang, U.A.Wiedemann Comparison of jet quenching formalisms for a quark-gluon plasma "brick"
doi: 10.1103/PhysRevC.86.064904
2012SA60 J.Phys.:Conf.Ser. 381, 012012 (2012) Hard probes of QCD matter at RHIC and the beginning of the LHC
doi: 10.1088/1742-6596/381/1/012012
2011ES01 Nucl.Phys. A855, 150c (2011) K.J.Eskola, H.Paukkunen, C.A.Salgado Nuclear PDFs at NLO - status report and review of the EPS09 results
doi: 10.1016/j.nuclphysa.2011.02.031
2011MI07 Nucl.Phys. A855, 494c (2011) J.G.Milhano, J.L.Albacete, N.Armesto, P.Quiroga-Arias, C.A.Salgado AAMQS: a non-linear phenomenological tool
doi: 10.1016/j.nuclphysa.2011.02.114
2009AR14 Nucl.Phys. A830, 271c (2009) N.Armesto, L.Cunqueiro, C.A.Salgado Monte Carlo for Jet Showers in the Medium
doi: 10.1016/j.nuclphysa.2009.10.098
2009ES03 Nucl.Phys. A830, 599c (2009) K.J.Eskola, H.Paukkunen, C.A.Salgado EPS09 - Global NLO Analysis of Nuclear PDFs and Their Uncertainties
doi: 10.1016/j.nuclphysa.2009.10.054
2007MA26 Phys.Lett. B 645, 138 (2007) L.Maiani, A.D.Polosa, V.Riquer, C.A.Salgado Counting valence quarks at RHIC and LHC NUCLEAR REACTIONS Au(Au, X), 1H(p, X), E=high; calculated nuclear modification factors, ratios. Comparison with data. Two component recombination/fragmentation model.
doi: 10.1016/j.physletb.2006.11.072
2007PO04 Nucl.Phys. A782, 305c (2007) Jets in opaque media at RHIC and LHC
doi: 10.1016/j.nuclphysa.2006.10.065
2007PO05 Phys.Rev. C 75, 041901 (2007) Jet shapes in opaque media
doi: 10.1103/PhysRevC.75.041901
2007PO12 J.Phys.(London) G34, S675 (2007) Double-humped jet structures within the radiative energy loss
doi: 10.1088/0954-3899/34/8/S71
2007SA09 Nucl.Phys. A783, 225c (2007) Suppression of Heavy Quarks at RHIC/LHC
doi: 10.1016/j.nuclphysa.2006.11.078
2007SA16 Nucl.Phys. A785, 85c (2007) Jets in Heavy Ion Collisions NUCLEAR REACTIONS 1H(p, X), 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed jet structure, related data.
doi: 10.1016/j.nuclphysa.2006.11.136
2007SA29 Acta Phys.Pol. B38, 975 (2007) Heavy ions theory review
2006AR10 Phys.Lett. B 637, 362 (2006) N.Armesto, M.Cacciari, A.Dainese, C.A.Salgado, U.A.Wiedemann How sensitive are high-pT electron spectra at RHIC to heavy quark energy loss? NUCLEAR REACTIONS 1H(p, X), E(cm)=200 GeV; Au(Au, X), E=high; calculated single inclusive electron spectra, nuclear modification factors and azimuthal asymmetry. Comparison with data.
doi: 10.1016/j.physletb.2005.12.073
2006AR22 J.Phys.(London) G32, S421 (2006) N.Armesto, M.Cacciari, A.Dainese, C.A.Salgado, U.A.Wiedemann Heavy quarks as a test of medium-induced energy loss at RHIC and at the LHC
doi: 10.1088/0954-3899/32/12/S51
2006AR27 Nucl.Phys. A774, 589 (2006) N.Armesto, M.Cacciari, A.Dainese, C.A.Salgado, U.A.Wiedemann Heavy-to-light ratios as a test of medium-induced energy loss at RHIC and the LHC NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; Pb(Pb, X), E(cm)=5.5 TeV/nucleon; calculated nuclear modification factors for heavy-flavored mesons, light-flavored hadrons and non-photonic electrons; analyzed nuclear modification factors heavy to light mass ratios. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.06.020
2006SA54 Nucl.Phys. A774, 267 (2006) RHIC results from LHC perspectives NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated nuclear modification factor, gluon multiplicity distributions, jet energy distributions, elliptic flow. Dokshitzer-Gribov-Lipatov-Alterelli-Parisi evolution equations, comparison with experimental data.
doi: 10.1016/j.nuclphysa.2006.06.047
2005AL05 Phys.Rev. D 71, 014003 (2005) J.L.Albacete, N.Armesto, J.G.Milhano, C.A.Salgado, U.A.Wiedemann Numerical analysis of the Balitsky-Kovchegov, equation with running coupling: Dependence of the saturation scale on nuclear size and rapidity
doi: 10.1103/PhysRevD.71.014003
2005AL35 Eur.Phys.J. C 43, 353 (2005) J.L.Albacete, N.Armesto, J.G.Milhano, C.A.Salgado, U.A.Wiedemann Nuclear size and rapidity dependence of the saturation scale from QCD evolution and experimental data
doi: 10.1140/epjc/s2005-02185-1
2005AR03 Phys.Rev.Lett. 94, 022002 (2005) N.Armesto, C.A.Salgado, U.A.Wiedemann Relating High-Energy Lepton-Hadron, Proton-Nucleus, and Nucleus-Nucleus Collisions through Geometric Scaling NUCLEAR REACTIONS 1H, Li, C, Ca, Pb(e, e'X), 197Au(197Au, X), (d, X), 1H(p-bar, X), E=high; analyzed geometric scaling features.
doi: 10.1103/PhysRevLett.94.022002
2005AR31 Phys.Rev. C 72, 064910 (2005) N.Armesto, C.A.Salgado, U.A.Wiedemann Low-pT collective flow induces high-pT jet quenching
doi: 10.1103/PhysRevC.72.064910
2005ES01 Nucl.Phys. A747, 511 (2005) K.J.Eskola, H.Honkanen, C.A.Salgado, U.A.Wiedemann The fragility of high-pT hadron spectra as a hard probe NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=62.4, 200 GeV/nucleon; Pb(Pb, X), E(cm)=5500 GeV/nucleon; calculated nuclear modification factors for charged hadron spectra.
doi: 10.1016/j.nuclphysa.2004.09.070
2004AR30 Phys.Rev.Lett. 93, 242301 (2004) N.Armesto, C.A.Salgado, U.A.Wiedmann Measuring the Collective Flow with Jets NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed jet energy distributions, particle correlations, sensitivity to collective flow.
doi: 10.1103/PhysRevLett.93.242301
2004SA34 Phys.Rev.Lett. 93, 042301 (2004) Medium Modification of Jet Shapes and Jet Multiplicities NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated jet shapes and multiplicity distributions, sensitivity to parton energy loss in dense medium.
doi: 10.1103/PhysRevLett.93.042301
2004SA37 J.Phys.(London) G30, S1295 (2004) Medium modification of the jet properties
doi: 10.1088/0954-3899/30/8/112
2003AR12 Eur.Phys.J. C 29, 531 (2003) N.Armesto, A.Capella, A.B.Kaidalov, J.Lopez-Albacete, C.A.Salgado Nuclear structure functions at small x from inelastic shadowing and diffraction NUCLEAR STRUCTURE 2H, He, Li, C, Ca, Sn, Pb; analyzed structure function data, shadowing effects. NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=19, 130, 200 GeV/nucleon; Pb(Pb, X), E(cm)=5500 GeV/nucleon; calculated multiplicity reduction factor.
doi: 10.1140/epjc/s2003-01243-0
2003ES05 Int.J.Mod.Phys. E12, 177 (2003) K.J.Eskola, H.Honkanen, V.J.Kolhinen, P.V.Ruuskanen, C.A.Salgado Nuclear Parton Distributions in the DGLAP Approach NUCLEAR STRUCTURE 4He, 9Be, 12C, 27Al, 40Ca, 56Fe, 117Sn, 208Pb; calculated parton distributions, nuclear medium modifications, related features. Perturbative QCD, various parameterizations compared.
doi: 10.1142/S0218301303001259
2003SA13 Nucl.Phys. A715, 783c (2003) Determining the BDMPS transport coefficient via medium-modified fragmentation functions
doi: 10.1016/S0375-9474(02)01488-4
2002ES05 Phys.Lett. 532B, 222 (2002) K.J.Eskola, H.Honkanen, V.J.Kolhinen, C.A.Salgado Constraints for Nuclear Gluon Shadowing from DIS Data NUCLEAR REACTIONS 12C, 117Sn(e, e'X), E not given; analyzed σ(x, Q2); deduced sensitivity to nuclear gluon distribution functions, gluon shadowing limit.
doi: 10.1016/S0370-2693(02)01592-7
2002SA36 Phys.Rev.Lett. 89, 092303 (2002) Dynamical Scaling Law for Jet Tomography
doi: 10.1103/PhysRevLett.89.092303
2001AR18 Phys.Lett. 520B, 124 (2001) A Geometrical Estimation of Saturation of Partonic Densities NUCLEAR REACTIONS 1H, Be, Fe, Pb(γ, X), E=high; calculated string densities.
doi: 10.1016/S0370-2693(01)01153-4
2001CA09 Phys.Rev. D63, 054010 (2001) A.Capella, E.G.Ferreiro, C.A.Salgado, A.B.Kaidalov Deep Inelastic Scattering Data and the Problem of Saturation in Small-x Physics NUCLEAR REACTIONS 1H(γ, X), E=high; calculated structure functions, σ for deep inelastic scattering; deduced unitarity effects.
doi: 10.1103/PhysRevD.63.054010
2001ES06 Eur.Phys.J. C 21, 613 (2001) K.J.Eskola, V.J.Kolhinen, C.A.Salgado, R.L.Thews Constraints for the Nuclear Sea Quark Distributions from the Drell-Yan Process at the SPS NUCLEAR REACTIONS 2H, Be, 184W(p, X), E(cm)=30 GeV; Pb(Pb, X), E=158 GeV/nucleon; calculated Drell-Yan production σ, related features; deduced role of nuclear effects in nucleon parton distributions.
doi: 10.1007/s100520100771
2001SA69 Phys.Lett. 521B, 211 (2001) xF-Dependence of J/ψ Suppression in pA Collisions
doi: 10.1016/S0370-2693(01)01162-5
1999BR05 Nucl.Phys. B(Proc.Supp.) S71, 254 (1999) M.A.Braun, C.Pajares, C.A.Salgado, N.Armesto, A.Capella Rescattering Effects in Heavy Flavour Production Off Nuclei NUCLEAR REACTIONS Pb(p, X), (Pb, X), E=20-6000 GeV; calculated effective atomic numbers for J/ψ, open charm production. Quantum field theoretical approach.
doi: 10.1016/S0920-5632(98)00351-X
1999CA30 Phys.Lett. 459B, 27 (1999) A.Capella, E.G.Ferreiro, C.A.Salgado Baryon and Antibaryon Production in Hadronic and Nuclear Interactions NUCLEAR REACTIONS Pb(p, X), (Pb, X), E=160 GeV/nucleon; calculated hyperon yields, rapidity densities; deduced final-state interactions contribution. Dual parton model.
doi: 10.1016/S0370-2693(99)00664-4
1999CA44 Phys.Rev. C60, 054906 (1999) Baryon Stopping and Hyperon Enhancement in the Improved Dual Parton Model NUCLEAR REACTIONS S(S, X), E at 200 GeV/c/nucleon; Pb(Pb, X), E at 158 GeV/c/nucleon; 197Au(p, X), E not given; calculated baryon, proton, hyperon yields, rapidity distributions. Improved dual parton model, comparisons with data.
doi: 10.1103/PhysRevC.60.054906
1999CA54 Nucl.Phys. A661, 502c (1999) A.Capella, E.G.Ferreiro, C.A.Salgado Baryon and Antibaryon Production in Hadronic and Nuclear Collisions
doi: 10.1016/S0375-9474(99)85075-1
1999ES06 Eur.Phys.J. C 9, 61 (1999) K.J.Eskola, V.J.Kolhinen, C.A.Salgado The Scale Dependent Nuclear Effects in Parton Distributions for Practical Applications
doi: 10.1007/s100520050513
1999ES08 Nucl.Phys. A661, 645c (1999) K.J.Eskola, V.J.Kolhinen, P.V.Ruuskanen, C.A.Salgado Nuclear Parton Distribution - a DGLAP Analysis
doi: 10.1016/S0375-9474(99)85108-2
1998AR02 Yad.Fiz. 61, No 1, 134 (1998); Phys.Atomic Nuclei 61, 125 (1998) N.Armesto, C.Pajares, C.A.Salgado, Yu.M.Shabelski A Dependences of the Cross Sections for Hard Processes in QCD NUCLEAR REACTIONS 197Au(p, X), (197Au, X), E=high; calculated heavy quark production σ.
1998PA25 Mod.Phys.Lett. A 13, 453 (1998) C.Pajares, C.A.Salgado, Yu.M.Shabelsky Nuclear Shadowing Effects on Charmonium Production in QCD NUCLEAR REACTIONS 197Au(p, X), (197Au, X), E(cm)=10-70 GeV; calculated J/ψ production color octet, singlet contributions.
doi: 10.1142/S0217732398000528
1997DI10 Phys.Lett. 408B, 417 (1997) J.Dias de Deus, C.Pajares, C.A.Salgado Production Associated to Rare Events in High Energy Hadron-Hadron Collisions NUCLEAR REACTIONS 1H(p-bar, X), E=high; analyzed W±-, Z0-production associated multiplicity distribution data, other aspects; deduced all hadronic processes similarity.
doi: 10.1016/S0370-2693(97)00815-0
1997DI12 Phys.Lett. 409B, 474 (1997) J.Dias de Deus, C.Pajares, C.A.Salgado Multiplicity and Transverse Energy Distributions Associated to Rare Events in Nucleus-Nucleus Collisions NUCLEAR REACTIONS U(S, X), Pb(Pb, X), E=high; analyzed J/Ψ production; deduced absorption, quark-gluon plasma formation roles.
doi: 10.1016/S0370-2693(97)00844-7
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