NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Jia Found 57 matches. 2023DI05 Eur.Phys.J. A 59, 45 (2023) Impact of nuclear shape fluctuations in high-energy heavy ion collisions
doi: 10.1140/epja/s10050-023-00965-1
2023JI01 Phys.Rev. C 107, L021901 (2023) Scaling approach to nuclear structure in high-energy heavy-ion collisions NUCLEAR REACTIONS 96Ru(96Ru, X), 96Zr(96Zr, X), √ s=200 GeV; analyzed observables of high-energy heavy-ion collision experiments - elliptic flow, triangular flow, charged particle multiplicity measured at RHIC (STAR collaboration); deduced difference of collective nuclear structure parameters for 96Ru and 96Zr isobars - quadrupole deformation parameter, octupole deformation parameter, half-density radius, surface diffuseness; calculated neutron skin thickness. Multiphase transport model (AMPT). Proposed scaling relation between collective nuclear structure parameters describing the shape and radial profiles of the nuclei and initial condition of the quark-gluon plasma (QGP) produced in heavy-ion collisions.
doi: 10.1103/PhysRevC.107.L021901
2023JI04 Chin.Phys.Lett. 40, 42501 (2023) Precision Tests of the Nonlinear Mode Coupling of Anisotropic Flow via High-Energy Collisions of Isobars NUCLEAR REACTIONS 96Ru(96Ru, X), 96Zr(96Zr, X), E not given; analyzed available data; deduced the nonlinear coupling between lower-order flow harmonics to the higher-order flow harmonics scale, scaling relations.
doi: 10.1088/0256-307X/40/4/042501
2023JI07 Phys.Rev.Lett. 131, 022301 (2023) Separating the Impact of Nuclear Skin and Nuclear Deformation in High-Energy Isobar Collisions NUCLEAR REACTIONS 95Ru(96Ru, X), 96Zr(96Zr, X), E not given; analyzed available data; deduced effects of nuclear skin thickness and nuclear deformations on the elliptic flow and its fluctuations.
doi: 10.1103/PhysRevLett.131.022301
2023LU18 Eur.Phys.J. A 59, 279 (2023) Z.Lu, M.Zhao, X.Li, J.Jia, Y.Zhou Probe nuclear structure using the anisotropic flow at the Large Hadron Collider
doi: 10.1140/epja/s10050-023-01194-2
2022BH02 Phys.Rev. C 105, 024904 (2022) Higher-order transverse momentum fluctuations in heavy-ion collisions
doi: 10.1103/PhysRevC.105.024904
2022JI01 Phys.Rev. C 105, 014905 (2022) Shape of atomic nuclei in heavy ion collisions NUCLEAR REACTIONS 96Zr(96Zr, X), 96Ru(96Ru, X), 129Xe(129Xe, X), 197Au(197Au, X), 208Pb(208Pb, X), 238U(238U, X), E=200 GeV; analyzed experimental data from RHIC-BNL and LHC-CERN for mean square eccentricities, and centralities as function of deformation parameters of ground states of colliding heavy ions using Monte Carlo Glauber model. 144,148,154Sm, 197Au, 198Hg, 208Pb, 238U; deduced correlation of mean square elliptic eccentricity and β2 deformation parameter for the ground states. 96Zr, 96Ru, 129Xe, 197Au, 208Pb, 238U; deduced β2, β3 and β4 deformation parameters for the ground states. Relevance to extraction of shapes of atomic nuclei in heavy ion collisions.
doi: 10.1103/PhysRevC.105.014905
2022JI02 Phys.Rev. C 105, 014906 (2022) Probing nuclear quadrupole deformation from correlation of elliptic flow and transverse momentum in heavy ion collisions NUCLEAR REACTIONS 197Au(197Au, X), 238U(238U, X), E=200 GeV; analyzed experimental data from RHIC-BNL and LHC-CERN for elliptic and radial flows, average transverse momentum as function of β2 quadrupole deformation parameter of ground states of colliding heavy ions using a multi-phase transport (AMPT) model, based on Monte Carlo Glauber initial conditions. Relevance to a precision tool to directly image the deformation of the atomic nuclei at extremely short timescale.
doi: 10.1103/PhysRevC.105.014906
2022JI06 Phys.Rev. C 105, 044905 (2022) Probing triaxial deformation of atomic nuclei in high-energy heavy ion collisions NUCLEAR REACTIONS 90Zr(90Zr, X), 238U(238U, X), E=200 GeV; analyzed experimental data from Relativistic Heavy-ion Collider (RHIC) and Large Hadron Collider (LHC) using for collective flow response of produced quark-gluon plasma to the eccentricity and the density gradient using analytical estimate and a Glauber model. 90Zr, 238U; deduced relevant coefficients in collisions of isobaric near prolate nuclei, ground state deformation parameters β2, (β2, γ) diagrams in heavy-ion collisions, β3, β4, and triaxial deformation.
doi: 10.1103/PhysRevC.105.044905
2022LI52 Phys.Rev. C 106, 034913 (2022) L.-M.Liu, C.-J.Zhang, J.Xu, J.Jia, G.-X.Peng Free spectator nucleons in ultracentral relativistic heavy-ion collisions as a probe of neutron skin NUCLEAR REACTIONS 96Zr(96Zr, X), 96Ru(96Ru, X), E(cm)=200 GeV; 197Au(197Au, X), E(cm)=130, 200 GeV; 208Pb(208Pb, X), E(cm)=5.02 TeV; analyzed experimental data from BNL-RHIC or LHC-CERN facilities; deduced deformation parameters β2, β3, neutron-skin thicknesses for different slope parameters, numbers of total spectator neutrons and protons, numbers of free spectator nucleons and light clusters, isospin asymmetries, Nn/Np ratios of free spectator neutrons to protons, average energy excitation per spectator nucleon as a function of charged-particle multiplicity. Skyrme-Hartree-Fock-Bogolyubov calculations, and Glauber model. Relevance to sensitive probe of the neutron-skin thickness and the slope parameter of the symmetry energy.
doi: 10.1103/PhysRevC.106.034913
2022LI55 Phys.Lett. B 834, 137441 (2022) L.-M.Liu, C.J.Zhang, J.Zhou, J.Xu, J.Jia, G.-X.Peng Probing neutron-skin thickness with free spectator neutrons in ultracentral high-energy isobaric collisions NUCLEAR REACTIONS 96Zr(96Zr, X), 96Ru(96Ru, X), E not given; analyzed available data; deduced the yield ratio of free spectator neutrons produced in high-energy collisions is a clean probe of the neutron-skin thickness of colliding nuclei and the slope parameter L of the symmetry energy based on state-of-the-art Skyrme-Hartree-Fock-Bogolyubov calculation.
doi: 10.1016/j.physletb.2022.137441
2022ZH02 Phys.Rev.Lett. 128, 022301 (2022) Evidence of Quadrupole and Octupole Deformations in 96Zr+96Zr and 96Ru+96Ru Collisions at Ultrarelativistic Energies NUCLEAR REACTIONS 96Zr(96Zr, X), 96Ru(96Ru, X), E not given; analyzed available data; deduced evidence of quadrupole and octupole deformations. STAR data.
doi: 10.1103/PhysRevLett.128.022301
2022ZH50 Phys.Rev. C 106, L031901 (2022) Ratios of collective flow observables in high-energy isobar collisions are insensitive to final-state interactions
doi: 10.1103/PhysRevC.106.L031901
2021AB12 Phys.Rev. C 104, L061901 (2021) M.S.Abdallah, B.E.Aboona, J.Adam, L.Adamczyk, J.R.Adams, J.K.Adkins, G.Agakishiev, I.Aggarwal, M.M.Aggarwal, Z.Ahammed, I.Alekseev, D.M.Anderson, A.Aparin, E.C.Aschenauer, M.U.Ashraf, F.G.Atetalla, A.Attri, G.S.Averichev, V.Bairathi, W.Baker, J.G.Ball Cap, K.Barish, A.Behera, R.Bellwied, P.Bhagat, A.Bhasin, J.Bielcik, J.Bielcikova, I.G.Bordyuzhin, J.D.Brandenburg, A.V.Brandin, I.Bunzarov, J.Butterworth, X.Z.Cai, H.Caines, M.Calderon de la Barca Sanchez, D.Cebra, I.Chakaberia, P.Chaloupka, B.K.Chan, F.-H.Chang, Z.Chang, N.Chankova-Bunzarova, A.Chatterjee, S.Chattopadhyay, D.Chen, J.Chen, J.H.Chen, X.Chen, Z.Chen, J.Cheng, M.Chevalier, S.Choudhury, W.Christie, X.Chu, H.J.Crawford, M.Csanad, M.Daugherity, T.G.Dedovich, I.M.Deppner, A.A.Derevschikov, A.Dhamija, L.Di Carlo, L.Didenko, P.Dixit, X.Dong, J.L.Drachenberg, E.Duckworth, J.C.Dunlop, N.Elsey, J.Engelage, G.Eppley, S.Esumi, O.Evdokimov, A.Ewigleben, O.Eyser, R.Fatemi, F.M.Fawzi, S.Fazio, P.Federic, J.Fedorisin, C.J.Feng, Y.Feng, P.Filip, E.Finch, Y.Fisyak, A.Francisco, C.Fu, L.Fulek, C.A.Gagliardi, T.Galatyuk, F.Geurts, N.Ghimire, A.Gibson, K.Gopal, X.Gou, D.Grosnick, A.Gupta, W.Guryn, A.I.Hamad, A.Hamed, Y.Han, S.Harabasz, M.D.Harasty, J.W.Harris, H.Harrison, S.He, W.He, X.H.He, Y.He, S.Heppelmann, S.Heppelmann, N.Herrmann, E.Hoffman, L.Holub, Y.Hu, H.Huang, H.Z.Huang, S.L.Huang, T.Huang, X.Huang, Y.Huang, T.J.Humanic, G.Igo, D.Isenhower, W.W.Jacobs, C.Jena, A.Jentsch, Y.Ji, J.Jia, K.Jiang, X.Ju, E.G.Judd, S.Kabana, M.L.Kabir, S.Kagamaster, D.Kalinkin, K.Kang, D.Kapukchyan, K.Kauder, H.W.Ke, D.Keane, A.Kechechyan, M.Kelsey, Y.V.Khyzhniak, D.P.Kikola, C.Kim, B.Kimelman, D.Kincses, I.Kisel, A.Kiselev, A.G.Knospe, H.S.Ko, L.Kochenda, L.K.Kosarzewski, L.Kramarik, P.Kravtsov, L.Kumar, S.Kumar, R.Kunnawalkam Elayavalli, J.H.Kwasizur, R.Lacey, S.Lan, J.M.Landgraf, J.Lauret, A.Lebedev, R.Lednicky, J.H.Lee, Y.H.Leung, C.Li, C.Li, W.Li, X.Li, Y.Li, X.Liang, Y.Liang, R.Licenik, T.Lin, Y.Lin, M.A.Lisa, F.Liu, H.Liu, H.Liu, P.Liu, T.Liu, X.Liu, Y.Liu, Z.Liu, T.Ljubicic, W.J.Llope, R.S.Longacre, E.Loyd, N.S.Lukow, X.F.Luo, L.Ma, R.Ma, Y.G.Ma, N.Magdy, D.Mallick, S.Margetis, C.Markert, H.S.Matis, J.A.Mazer, N.G.Minaev, S.Mioduszewski, B.Mohanty, M.M.Mondal, I.Mooney, D.A.Morozov, A.Mukherjee, M.Nagy, J.D.Nam, Md.Nasim, K.Nayak, D.Neff, J.M.Nelson, D.B.Nemes, M.Nie, G.Nigmatkulov, T.Niida, R.Nishitani, L.V.Nogach, T.Nonaka, A.S.Nunes, G.Odyniec, A.Ogawa, S.Oh, V.A.Okorokov, B.S.Page, R.Pak, J.Pan, A.Pandav, A.K.Pandey, Y.Panebratsev, P.Parfenov, B.Pawlik, D.Pawlowska, H.Pei, C.Perkins, L.Pinsky, R.L.Pinter, J.Pluta, B.R.Pokhrel, G.Ponimatkin, J.Porter, M.Posik, V.Prozorova, N.K.Pruthi, M.Przybycien, J.Putschke, H.Qiu, A.Quintero, C.Racz, S.K.Radhakrishnan, N.Raha, R.L.Ray, R.Reed, H.G.Ritter, M.Robotkova, O.V.Rogachevskiy, J.L.Romero, D.Roy, L.Ruan, J.Rusnak, N.R.Sahoo, H.Sako, S.Salur, J.Sandweiss, S.Sato, W.B.Schmidke, N.Schmitz, B.R.Schweid, F.Seck, J.Seger, M.Sergeeva, R.Seto, P.Seyboth, N.Shah, E.Shahaliev, P.V.Shanmuganathan, M.Shao, T.Shao, A.I.Sheikh, D.Shen, S.S.Shi, Y.Shi, Q.Y.Shou, E.P.Sichtermann, R.Sikora, M.Simko, J.Singh, S.Singha, M.J.Skoby, N.Smirnov, Y.Sohngen, W.Solyst, P.Sorensen, H.M.Spinka, B.Srivastava, T.D.S.Stanislaus, M.Stefaniak, D.J.Stewart, M.Strikhanov, B.Stringfellow, A.A.P.Suaide, M.Sumbera, B.Summa, X.M.Sun, X.Sun, Y.Sun, Y.Sun, B.Surrow, D.N.Svirida, Z.W.Sweger, P.Szymanski, A.H.Tang, Z.Tang, A.Taranenko, T.Tarnowsky, J.H.Thomas, A.R.Timmins, D.Tlusty, T.Todoroki, M.Tokarev, C.A.Tomkiel, S.Trentalange, R.E.Tribble, P.Tribedy, S.K.Tripathy, T.Truhlar, B.A.Trzeciak, O.D.Tsai, Z.Tu, T.Ullrich, D.G.Underwood, I.Upsal, G.Van Buren, J.Vanek, A.N.Vasiliev, I.Vassiliev, V.Verkest, F.Videbaek, S.Vokal, S.A.Voloshin, F.Wang, G.Wang, J.S.Wang, P.Wang, Y.Wang, Y.Wang, Z.Wang, J.C.Webb, P.C.Weidenkaff, L.Wen, G.D.Westfall, H.Wieman, S.W.Wissink, J.Wu, Y.Wu, B.Xi, Z.G.Xiao, G.Xie, W.Xie, H.Xu, N.Xu, Q.H.Xu, Y.Xu, Z.Xu, Z.Xu, C.Yang, Q.Yang, S.Yang, Y.Yang, Z.Ye, Z.Ye, L.Yi, K.Yip, Y.Yu, H.Zbroszczyk, W.Zha, C.Zhang, D.Zhang, J.Zhang, S.Zhang, S.Zhang, X.P.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, Z.J.Zhang, Z.Zhang, Z.Zhang, J.Zhao, C.Zhou, X.Zhu, M.Zurek, M.Zyzak Global Λ-hyperon polarization in Au+Au collisions at √ sNN = 3 GeV
doi: 10.1103/PhysRevC.104.L061901
2021GI13 Phys.Rev. C 104, L041903 (2021) Accessing the shape of atomic nuclei with relativistic collisions of isobars NUCLEAR STRUCTURE 96Ru, 96Zr, 154Sm, 154Gd, 150Sm, 150Nd; analyzed probe for determining small differences in quadrupole and octupole deformations for pairs of isobaric nuclei in relativistic heavy-ion collision experiments, an overlap between low- and high-energy nuclear physics, as established in recent experiments at RHIC-BNL and at LHC-CERN by observing strong effects of deformation of the colliding ions on the output of relativistic nuclear collisions. Discussed recent experimental results for ratios of flow coefficients in 96Zr+96Zr and 96Ru+96Ru collisions from STAR collaboration at RHIC-BNL and consistency with low-energy spectroscopic measurements identifying a low-lying 3- state with a large B(E3) strength in such nuclei. Relevance to precise geometric shapes of nuclei and critically evaluations of low-energy nuclear structure data. Pairs of relevant stable isobars with large (β2>0.2) deformations: 36Ar-36S, 40Ca-40Ar, 46,48Ca-46,48Ti, 50Ti-50V-50Cr, 54Cr-54Fe, 64Ni-64Zn, 70Zn-70Ge, 74,76Ge-74,76Se, 78,80Se-78,80Kr, 84Kr-84Sr-84Mo, 86Kr-86Sr, 87Rb-87Sr, 92Zr-92Nb-92Mo, 94Zr-94Mo, 96Zr-96Mo-96Mo, 98,100Mo-98,100Ru, 100,102Ru-100,102Pd, 106,108,110Pd-106,108,110Cd, 112,114,116Cd-112,114,116Sn, 114Cd-114In, 115In-115Sn, 120,122Sn-120,122Te, 123Sb-123Te, 124Sn-124Te-124Xe, 126,128Te-126,128Xe, 130Te-130Xe-130Ba, 132,134Xe-132,134Ba, 136Xe-136Ba-136Ce, 138Ba-138La-138Ce, 142Ce-142Nd, 144,146,148,150Nd-144,146,148,150Sm, 152,154Sm-152,154Gd, 156,158,160Gd-156,158,160Dy, 162,164Dy-162,164Er, 168,170Er-168,170Yb, 174Er-174Hf, 176Yb-176Lu-176Hf, 180Hf-180W, 184,186W-184,186Os, 187Re-187Os, 190,192Os-190,192Pt, 198Pt-198Pt, and 204Hg-204Pb. Also, ground-state octupole deformation for some pairs of A=146, 148 and 150 nuclei.
doi: 10.1103/PhysRevC.104.L041903
2021GI17 Phys.Rev.Lett. 127, 242301 (2021) Impact of Nuclear Deformation on Relativistic Heavy-Ion Collisions: Assessing Consistency in Nuclear Physics across Energy Scales NUCLEAR REACTIONS 238U(238U, X), 197Au(197Au, X), E not given; analyzed available data; deduced formula based on generic scaling laws of hydrodynamics to relate the difference in elliptic flow measured between collision systems that are close in size to the value of deformation of the respective species. Collisions at top Relativistic Heavy Ion Collider (RHIC) energy.
doi: 10.1103/PhysRevLett.127.242301
2021JI01 Nucl.Phys. A1005, 121761 (2021) J.Jia, for the ATLAS Collaboration Flow and centrality fluctuations from ATLAS
doi: 10.1016/j.nuclphysa.2020.121761
2021JI04 Phys.Rev. C 103, 024314 (2021) Systematics of α-decay energies in the valence correlation scheme RADIOACTIVITY 248,249,250,251,252,253,254,255,256No, 251,252,253,254,255,256,257,258,259Lr, 253,254,255,256,257,258Rf, 277,285Cn, 284,285,286Nh, 284,285,286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated Q(α) from analysis of evaluated Q(α) data for Z=52-118 nuclei in AME2016 using a simple valence correlation scheme (VCS), and compared with available experimental data.
doi: 10.1103/PhysRevC.103.024314
2021JI12 Phys.Rev. C 104, L031301 (2021) Possible cluster states in heavy and superheavy nuclei NUCLEAR STRUCTURE 20Ne, 44Ti, 94Mo, 104Te, 212Po; calculated level energies of positive-parity yrast levels and B(E2) up to 8+ in 20Ne, 12+ in 44Ti, 94Mo and 104Te, and 10+ in 212Po. 222Ra, 236Pu; calculated level energies of positive-parity yrast levels up to 12+. Calculations used binary (α+core) cluster model (BCM) and improved version of this model (IBCM). Comparison with available experimental data. 282Cn; discussed recently observed first 2+ state in 282Cn in terms of IBCM calculations.
doi: 10.1103/PhysRevC.104.L031301
2020HU02 Phys.Rev. C 101, 021901 (2020) Disentangling contributions to small-system collectivity via scans of light nucleus-nucleus collisions
doi: 10.1103/PhysRevC.101.021901
2020LI29 Phys.Rev. C 102, 024911 (2020) Z.Liu, A.Behera, H.Song, J.Jia Robustness of principal component analysis of harmonic flow in heavy ion collisions
doi: 10.1103/PhysRevC.102.024911
2019NI14 Phys.Rev. C 100, 064905 (2019) M.Nie, L.Yi, X.Luo, G.Ma, J.Jia Influence of initial-state momentum anisotropy on the final-state collectivity in small collision systems
doi: 10.1103/PhysRevC.100.064905
2018NI11 Phys.Rev. C 98, 034903 (2018) M.-W.Nie, Pe.Huo, J.Jia, G.-L.Ma Multiparticle azimuthal cumulants in p + Pb collisions from a multiphase transport model
doi: 10.1103/PhysRevC.98.034903
2018ZH45 Phys.Rev. C 98, 044903 (2018) Centrality fluctuations in heavy-ion collisions
doi: 10.1103/PhysRevC.98.044903
2017JI02 J.Phys.(London) G44, 075106 (2017) Observables for longitudinal flow correlations in heavy-ion collisions
doi: 10.1088/1361-6471/aa74c3
2017JI05 Phys.Rev. C 96, 034906 (2017) Revealing long-range multiparticle collectivity in small collision systems via subevent cumulants
doi: 10.1103/PhysRevC.96.034906
2017JI06 Nucl.Phys. A967, 51 (2017) J.Jia, for the ATLAS Collaboration Heavy Ion Results from ATLAS
doi: 10.1016/j.nuclphysa.2017.05.076
2016JI03 Phys.Rev. C 93, 044905 (2016) J.Jia, S.Radhakrishnan, M.Zhou Forward-backward multiplicity fluctuation and longitudinal harmonics in high-energy nuclear collisions
doi: 10.1103/PhysRevC.93.044905
2016JI10 Nucl.Phys. A956, 401 (2016) J.Jia, S.Radhakrishnan, M.Zhou, Pe.Huo Forward-backward multiplicity fluctuation and longitudinal harmonics in high-energy nuclear collisions
doi: 10.1016/j.nuclphysa.2016.02.069
2016JI11 Nucl.Phys. A956, 405 (2016) J.Jia, ATLAS Collaboration Forward-backward multiplicity correlations in pp, p+Pb and Pb+Pb collisions with the ATLAS detector
doi: 10.1016/j.nuclphysa.2016.02.069
2015JI10 Phys.Rev. C 92, 024911 (2015) Limitation of multiparticle correlations for studying the event-by-event distribution of harmonic flow in heavy-ion collisions
doi: 10.1103/PhysRevC.92.024911
2014HU15 Phys.Rev. C 90, 024910 (2014) Elucidating the event-by-event flow fluctuations in heavy-ion collisions via the event-shape selection technique
doi: 10.1103/PhysRevC.90.024910
2014JI09 Phys.Rev. C 90, 034905 (2014) Method for studying the rapidity fluctuation and de-correlation of harmonic flow in heavy-ion collisions
doi: 10.1103/PhysRevC.90.034905
2014JI10 Phys.Rev. C 90, 034915 (2014) Forward-backward eccentricity and participant-plane angle fluctuations and their influences on longitudinal dynamics of collective flow
doi: 10.1103/PhysRevC.90.034915
2014LA05 Phys.Rev.Lett. 112, 082302 (2014) R.A.Lacey, A.Taranenko, J.Jia, D.Reynolds, N.N.Ajitanand, J.M.Alexander, Y.Gu, A.Mwai Beam Energy Dependence of the Viscous Damping of Anisotropic Flow in Relativistic Heavy Ion Collisions
doi: 10.1103/PhysRevLett.112.082302
2013JI06 Nucl.Phys. A904-905, 421c (2013) J.Jia, for the ATLAS Collaboration Measurement of event-by-event flow harmonics in Pb-Pb Collisions at √ sNN = 2.76 TeV with the ATLAS detector
doi: 10.1016/j.nuclphysa.2013.02.039
2013JI07 Phys.Rev. C 87, 061901 (2013) Azimuthal anisotropy in a jet absorption model with fluctuating initial geometry in heavy ion collisions
doi: 10.1103/PhysRevC.87.061901
2013JI09 Phys.Rev. C 88, 014907 (2013) Disentangling flow and nonflow correlations via Bayesian unfolding of the event-by-event distributions of harmonic coefficients in ultrarelativistic heavy-ion collisions
doi: 10.1103/PhysRevC.88.014907
2013JI11 J.Phys.(London) G40, 105108 (2013) J.Jia, S.Radhakrishnan, S.Mohapatra A study of the anisotropy associated with dipole asymmetry in heavy ion collisions
doi: 10.1088/0954-3899/40/10/105108
2013JI14 Nucl.Phys. 910-911, 276c (2013) J.Jia, for the ATLAS Collaboration Measurement of Event Plane Correlations in Pb-Pb Collisions at √ sNN=2.76 TeV with the ATLAS Detector
doi: 10.1016/j.nuclphysa.2012.12.043
2011JI05 Nucl.Phys. A855, 92c (2011) J.Jia, for the PHENIX Collaboration Zeroing in on jet quenching: a PHENIX perspective
doi: 10.1016/j.nuclphysa.2011.02.024
2011JI09 Phys.Rev. C 84, 034904 (2011) Correlations between jet-quenching observables at energies available at the BNL Relativistic Heavy Ion Collider
doi: 10.1103/PhysRevC.84.034904
2011LA07 Phys.Rev. C 83, 044902 (2011) R.A.Lacey, R.Wei, J.Jia, N.N.Ajitanand, J.M.Alexander, A.Taranenko Initial eccentricity fluctuations and their relation to higher-order flow harmonics
doi: 10.1103/PhysRevC.83.044902
2011LA12 Phys.Rev. C 84, 027901 (2011) R.A.Lacey, R.Wei, N.N.Ajitanand, J.M.Alexander, J.Jia, A.Taranenko Glauber-based evaluations of the odd moments of the initial eccentricity relative to the even order participant planes
doi: 10.1103/PhysRevC.84.027901
2010JI08 Nucl.Phys. A834, 229c (2010) Probing the properties of the strongly-interacting quark gluon plasma at RHIC
doi: 10.1016/j.nuclphysa.2009.12.047
2010JI09 Phys.Rev. C 82, 024902 (2010) Dissecting the role of initial collision geometry for jet quenching observables in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.82.024902
2010LA03 Phys.Rev. C 81, 061901 (2010) R.A.Lacey, R.Wei, N.N.Ajitanand, J.M.Alexander, X.Gong, J.Jia, A.Taranenko, R.Pak, H.Stocker Constraints on models for the initial collision geometry in ultrarelativistic heavy ion collisions
doi: 10.1103/PhysRevC.81.061901
2010LA13 Phys.Rev. C 82, 034910 (2010) R.A.Lacey, A.Taranenko, R.Wei, N.N.Ajitanand, J.M.Alexander, J.Jia, R.Pak, D.H.Rischke, D.Teaney, K.Dusling Azimuthal anisotropy: Transition from hydrodynamic flow to jet suppression
doi: 10.1103/PhysRevC.82.034910
2009JI01 Phys.Rev. C 79, 011901 (2009) Influence of quenched jets on di-hadron correlations
doi: 10.1103/PhysRevC.79.011901
2009JI05 Phys.Rev.Lett. 103, 022301 (2009) Away-Side Asymmetry of Jet Correlation Relative to the Reaction Plane: A Sensitive Probe for Jet In-Medium Modifications
doi: 10.1103/PhysRevLett.103.022301
2009LA19 Phys.Rev.Lett. 103, 142302 (2009) R.A.Lacey, R.Wei, N.N.Ajitanand, J.M.Alexander, X.Gong, J.Jia, A.Mawi, S.Mohapatra, D.Reynolds, S.Salnikov, A.Taranenko Energy Loss for Heavy Quarks in Relation to Light Partons: Is Radiative Energy Loss for Heavy Quarks Anomalous?
doi: 10.1103/PhysRevLett.103.142302
2009LA29 Phys.Rev. C 80, 051901 (2009) R.A.Lacey, N.N.Ajitanand, J.M.Alexander, X.Gong, J.Jia, A.Taranenko, R.Wei Scaling patterns of the suppression of π0 yields in Au+Au collisions at √ sNN = 200 GeV: Links to the transport properties of the QGP
doi: 10.1103/PhysRevC.80.051901
2007JI03 Nucl.Phys. A783, 501c (2007) J.Jia, for the PHENIX Collaboration Ways to Constrain the Away-side Jet in Au + Au Collisions in PHENIX NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed dijet correlations, elliptic flow.
doi: 10.1016/j.nuclphysa.2006.11.104
2007JI04 Phys.Rev. C 75, 031901 (2007) Quark number scaling of v2 in transverse kinetic energy and its implications for coalescence models
doi: 10.1103/PhysRevC.75.031901
2005DR03 Phys.Rev. C 71, 034909 (2005) Medium-induced jet absorption in relativistic heavy-ion collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated particle yields vs centrality, role of medium-induced jet absorption.
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