Chunjian Zhang’s research while affiliated with Stony Brook University and other places

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Publications (24)


FIG. 1. Ratios of v 2 3 between 238 U+ 238 U and 197 Au+ 197 Au collisions as a function of centrality for different β3 values from the IP-Glasma+MUSIC+UrQMD calculations. The shaded bands denote the statistical uncertainties. The dashed box marked the 0-2% centrality range that is most sensitive to β3.
FIG. 2. Predicted v 2 3,U / v 2 3,Au as a function of β 2 3,U assuming β 2 3,Au = 0 from the IP-Glasma+MUSIC+UrQMD model for 0−2% centrality. The arrows indicate the corresponding values corresponding to β 2 3,U = 0.078 and 0.10 from Refs. [25, 28].
FIG. 3. Ratios of ⟨v 2 3 δpT⟩ between 238 U+ 238 U and 197 Au+ 197 Au collisions as a function of centrality for different values of β3,U from the IP-Glasma+MUSIC+UrQMD hydrodynamic model calculations. The shaded bands denote the statistical uncertainties.
FIG. 4. Centrality dependence of ratios of v 2 3 (panel a) and ⟨v 2 3 δpT⟩ (panel b) between 238 U+ 238 U and 197 Au+ 197 Au collisions from the IP-Glasma+MUSIC+UrQMD model for four pT intervals. The shaded bands denote the statistical uncertainties.
Probing the octupole deformation of 238^{238}U in high-energy nuclear collisions
  • Preprint
  • File available

April 2025

Chunjian Zhang

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Jiangyong Jia

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Jinhui Chen

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[...]

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Lumeng Liu

Some atomic nuclei exhibit ``pear" shapes arising from octupole deformation (β3\beta_3), though direct experimental evidences for such exotic shapes remains scarce. Low-energy model studies suggest 238^{238}U may have a modest octupole deformation arising from collective vibrational degrees of freedom, in addition to a large prolate shape. We investigated the impact of this modest octupole shape on observables involving triangular flow (v3v_3) in high-energy nuclear collisions. Using a hydrodynamic framework, we show v3v_3 and its correlation with mean transverse momentum, \langle v_3^2 \delta\pT \rangle, exhibit strong sensitivity to β3\beta_3. We found that v32\langle v_3^2\rangle follows a linear increase with β32\beta_3^2, while \langle v_3^2 \delta\pT \rangle is suppressed in the presence of β3\beta_3. Our findings show that the collective-flow-assisted nuclear imaging method in high-energy nuclear collisions, when compared with experimental data, can provide unique constraints on higher-order deformations.

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FIG. 1. (a): Bowling-pin configuration of 20 Ne with five α clusters; (b): Realistic density distribution of 20 Ne with α clusters; (c): Fitted density distribution of 20 Ne with a deformed WS form.
FIG. 2. Mid-rapidity observables (⟨p T ⟩, ⟨v 2 n ⟩, ⟨δp 2 T ⟩, and ⟨v 2 n δp T ⟩) at 0 − 20% centrality in 20 Ne+ 20 Ne collisions at √ s NN = 200 GeV [(a)-(f)] and 7 TeV [(g)-(l)] from the realistic and deformed WS density distributions shown in Fig. 1.
FIG. 3. Yield of spectator neutrons (a), protons (b), deuterons (c), tritons (d), 3 He (e), and α particles (f) as well as the corresponding yield ratios of free spectator neutrons to charged particles with mass-to-charge ratio A/Z = 3 (g), 3/2 (h), and 2 (i) scaled by their constituent nucleon numbers, at 0 − 20% centrality in 20 Ne + 20 Ne collisions at √ s NN = 200 GeV. The bars and symbols represent results with and without the deexcitation process, respectively.
FIG. 4. Similar to Fig. 3 but for 20 Ne+ 20 Ne collisions at √ s NN = 7 TeV.
Directly probing existence of α\alpha-cluster structure in 20^{20}Ne by relativistic heavy-ion collisions

February 2025

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13 Reads

Can relativistic heavy-ion collisions only probe the global shape of colliding nuclei, or their detailed internal structure as well? Taking 20^{20}Ne as an example, we attempt to directly probe its internal α\alpha-cluster structure, by comparing experimentally measured observables in collisions at relativistic energies from density distributions of 20^{20}Ne with and without α\alpha-cluster structure. Since the two density distributions give the same nucleus size and deformation, they lead to similar mid-rapidity observables. However, the α\alpha-cluster structure may considerably reduce the free spectator nucleon yield and enhance the spectator light nuclei yield, as a result of more compact initial phase-space distribution of nucleons inside α\alpha clusters. We propose to measure the scaled yield ratio of free spectator neutrons to charged particles with mass-to-charge ratio A/Z=3A/Z = 3, 3/2, and 2 in ultra-central \nene\ collisions, which is found to be reduced by about 25%25\% at sNN=7\sqrt{s_\mathrm{NN}} = 7 TeV and about 20\% at sNN=200\sqrt{s_\mathrm{NN}} = 200 GeV with α\alpha-cluster structure in 20^{20}Ne. This scaled yield ratio thus serves as a robust and direct probe of the existence of α\alpha-cluster structure in 20^{20}Ne free from the uncertainty of mid-rapidity dynamics.



FIG. 7. (Color online) The scaled variance k2 is calculated for Au+Au collisions as a function of ⟨Npart⟩ at 19.6 GeV using three configurations: the standard method in default (Def-AMPT), normal string-melting (SM-AMPT), and string-melting without partonic interactions (SM-AMPT: σp = 0 mb).
Energy dependence of transverse momentum fluctuations in Au+Au collisions from a multiphase transport model

January 2025

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5 Reads

Event-by-event mean transverse momentum fluctuations (pT\langle p_\mathrm{T}\rangle) serve as a sensitive probe of initial state overlap geometry and energy density fluctuations in relativistic heavy-ion collisions. We present a systematic investigation of pT\langle p_\mathrm{T}\rangle fluctuations in \auau collisions at sNN=\mathrm{\sqrt{s_{NN}}} =3.0-19.6 GeV, examining their centrality and energy dependence with the framework of an improved multiphase transport (AMPT) model. The centrality dependence of the pTp_\mathrm{T} cumulants up to fourth order deviates significantly from simple powering-law scaling. Scaled cumulants are performed, with variances aligning well with the trends observed in the experimental data. Employing a two-subevent method, short-range correlations are slightly suppressed compared to the standard approach. Furthermore, baryons exhibit more pronounced pT\langle p_\mathrm{T}\rangle fluctuations than mesons, potentially attributable to the effect of radial flow. These results provide referenced insights into the role of initial state fluctuations across different energies in heavy-ion collisions.


FIG. 1. (a) The mass data were selected from the AME2020 and AME2016 datasets, with Z, N > 20, and only the nuclei with experimental errors less than 100 keV were used. (b) The mass data were selected from the AME2020 dataset for nuclei with Z, N > 20, and only the nuclei with experimental errors less than 100 keV were used. For superheavy elements (Z > 94), predictions were supplemented using the WS4 model.
Validation and extrapolation of atomic mass with physics-informed fully connected neural network

January 2025

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19 Reads

Machine learning offers a powerful framework for validating and predicting atomic mass. We compare three improved neural network methods for representation and extrapolation for atomic mass prediction. The powerful method, adopting a macroscopic-microscopic approach and treating complex nuclear effects as output labels, achieves superior accuracy in AME2020, yielding a much lower root-mean-square deviation of 0.122 MeV in the test set, significantly lower than alternative methods. It also exhibits a better extrapolation performance when predicting AME2020 from AME2016, with a root-mean-square deviation of 0.191 MeV. We further conduct sensitivity analyses against the model inputs to verify interpretable alignment beyond statistical metrics. Incorporating theoretical predictions of magic numbers and masses, our fully connected neural networks reproduce key nuclear phenomena including nucleon pairing correlation and magic number effects. The extrapolation capability of the framework is discussed and the accuracy of predicting new mass measurements for isotope chains has also been tested.


Fig. 1 Asymmetric cumulant asc nm,n+m {3} representing the influence of nuclear structures as a function of N part in 0.2 < p T < 2 GeV/c in isobaric collisions. The effects of various Woods-Saxon parameters in Table. 1 are shown.
Fig. 2 Nonlinear coupling coefficients χ 4 (left panel) and χ 5 representing the influence of nuclear structures as a function of N part in 0.2 < p T < 2 GeV/c in isobaric collisions. The effects of various Woods-Saxon parameters in Table. 1 are shown.
Nuclear structure parameters in Eq. (1) used in the simulations of 96 Ru+ 96 Ru and 96 Zr+ 96 Zr collisions at √ s NN = 200 GeV. Case1 and Case5 represent, respectively, the full parameterizations of 96 Ru and 96 Zr.
Multiparticle azimuthal correlations in isobaric 96^{96}Ru+96^{96}Ru and 96^{96}Zr+96^{96}Zr collisions at sNN=\sqrt{s_{NN}} = 200 GeV

September 2024

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11 Reads

Correlations between event-by-event fluctuations in the amplitudes of flow harmonics offer a novel way to access initial state properties in heavy-ion collisions. We have extensively predicted correlations in different flow harmonics based on multiparticle cumulants in 96^{96}Ru+96^{96}Ru and 96^{96}Zr+96^{96}Zr collisions at sNN=\sqrt{s_{NN}} = 200 GeV from a multiphase transport model. The state-of-the-art correlated nuclear distributions for the isobars were used to show the difference in nuclear deformations and neutron skin thickness, which have distinct characteristics seen in multiparticle azimuthal correlation. We also found a minimal effect of the shear viscosity effect on these multiparticle azimuthal correlations. Therefore, these studies could also serve as an additional tool for understanding the nature of the initial state fluctuations and nuclear structure, as well as input for possible in-depth dynamical studies for experimental measurement.


Citations (9)


... In recent years, high-energy scattering experiments have emerged as a new tool for probing nuclear deformations [6]. Quite remarkably, collective flow measurements in high-energy nuclear collisions reveal a rather strong dependence on the lowenergy structure of the colliding ions [7,8,9,10,11,12,13,14,15], showing sensitivity to their shapes [16,17,18,19,20,21,22,23,24,25,26], their skin thickness [27,28,29,30], and potential clustering phenomena [31,32,33,34,35]. Similarly, deep inelastic scattering in γA collisions is also sensitive to the nuclear structure [36,37,38,39]. ...

Reference:

Angular structure of many-body correlations in atomic nuclei: From nuclear deformations to diffractive vector meson production in $\gamma A$ collisions
Directly probing existence of α -cluster structure in Ne 20 by relativistic heavy-ion collisions
  • Citing Article
  • February 2025

Physical Review C

... In Fig. 2 panel (b), the regions labeled ePIC-I, ePIC-II, and ePIC-III correspond to the acceptance ranges of the three primary subsystems anticipated for the eP IC detector [23], which are the focus of this study. Beyond these intrinsic capabilities of the EIC, we propose utilizing event-by-event fluctuations in the mean transverse momentum (M (p T )) as a measurement to constrain the τ f effect in e+A collisions [28][29][30]. Specifically, M (p T ) fluctuations encode information about the origin of emitted particles: the de-excitation stage tends to yield more thermal-like, isotropic, and statistically narrow momentum distributions, whereas the intranuclear cascade phase leads to broader and more irregular distributions due to the stochastic and non-thermal character of secondary particle interactions. Thus, M (p T ) fluctuations are expected to serve as a sensitive probe of the underlying particle production mechanism, which is anticipated to depend on τ f . ...

Energy dependence of transverse momentum fluctuations in Au + Au collisions from a multiphase transport model
  • Citing Article
  • February 2025

Physical Review C

... According to the low energy experiments, 16 O nucleus exhibit a tetrahedral structure with alpha-clusters at its edges [370,221] shown in Fig. (7.2). As a result there exist surging theoretical interest to image the structure of 16 O nucleus and study its unique collective signatures in high-energy O+O collision [371,370,221,[372][373][374][375]. The measurements from the STAR collaboration highlight significant contributions from sub-nucleonic fluctuations and nucleon-nucleon correlation at the initial state of O+O collision. ...

Ab-initio nucleon-nucleon correlations and their impact on high energy 16O+16O collisions
  • Citing Article
  • February 2025

Physics Letters B

... A robust imaging method is essential for disentangling and studying each contribution separately. By comparing results from RHIC and the LHC, one can investigate the energy dependence of these two components in detail [9]. Reverse-engineering nuclear shape A nucleus with quadrupole deformation can be described by a surface function in terms of the polar angle θ and azimuthal angle ϕ, R(θ, ϕ) = R 0 (1 + β 2 (cos γY 2,0 + sin γY 2,2 )) , (1) where Y l,m (θ, ϕ) are spherical harmonics. ...

Energy dependence of heavy-ion initial condition in isobar collisions
  • Citing Article
  • September 2024

Physics Letters B

... High-energy heavy-ion collisions offer a unique opportunity to probe the structure of atomic nuclei [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17]. The much shorter time scale of these reactions (10 −24 s) compared to traditional low-energy studies (10 −21 s) allows for the exploration of nuclear shapes and the nucleon distribution within the nucleus [6,7,18]. ...

Impact of nuclear structure on longitudinal flow decorrelations in high-energy isobar collisions
  • Citing Article
  • September 2023

Physics Letters B

... We investigate the signal of the chiral magnetic effect (CME) in Au + Au collisions and isobar collisions of 96 44 Ru + 96 44 Ru and 96 40 Zr + 96 40 Zr in the newly developed chiral anomaly transport module based on the state-ofthe-art model "a multiphase transport." Our numerical simulation results for the ratio charge correlation γ in Ru + Ru and Zr + Zr collisions are close to the latest experimental data. ...

Separating the Impact of Nuclear Skin and Nuclear Deformation in High-Energy Isobar Collisions
  • Citing Article
  • July 2023

Physical Review Letters

... At the other end of the energy spectrum, collider studies have established that measurements of the collective flow of hadrons in the soft sector of high-energy nuclear collisions enable us to experimentally access fine properties of the shapes and radial distributions of nuclei in their ground states [29][30][31][32][33][34][35][36][37]. In particular, by studying how observables such as anisotropic flow coefficients vary across collision systems involving isobaric isotopes [38], one can measure signatures of the structure of these nuclei while drastically mitigating the impact of theoretical uncertainties on poorly understood features of the QGP, such as out-of-equilibrium or hadronization phenomena, in the interpretation of the data [39][40][41][42][43][44][45][46][47]. Therefore, collider experiments with isobars provide robust probes of the nuclear geometry, and since 0νββ decay is expected to occur between two isobaric ground states, it is natural to leverage this new knowledge to assess how high-energy experiments constrain model determinations of the NME. ...

Ratios of collective flow observables in high-energy isobar collisions are insensitive to final-state interactions
  • Citing Article
  • September 2022

Physical Review C

... Moreover, in the past few years, isobar collisions such as Zr+Zr and Ru+Ru were introduced to explore atomic nuclei's skin and shape. The quantitative analysis becomes feasible as the relevant bulk observables such as v 2 and v 3 ratios have been obtained with unprecedented precision [43][44][45][46][47][48][49]. Besides, these isobars collisions are distinct in terms of the shapes of the participant nuclei, which are characterized by different deformations. ...

Impact of event activity variable on the ratio observables in isobar collisions
  • Citing Article
  • July 2022

Physics Letters B