J. Scott Moreland’s research while affiliated with Duke University and other places

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Publications (28)


Bayesian calibration of a hybrid nuclear collision model using p − Pb and Pb-Pb data at energies available at the CERN Large Hadron Collider
  • Article

February 2020

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43 Reads

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158 Citations

Physical Review C

J. Scott Moreland

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Jonah E. Bernhard

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Steffen A. Bass

We posit a unified hydrodynamic and microscopic description of the quark-gluon plasma (QGP) produced in ultrarelativistic p−Pb and Pb-Pb collisions at sNN=5.02TeV and evaluate our assertion using Bayesian inference. Specifically, we model the dynamics of both collision systems using initial conditions with parametric nucleon substructure, a preequilibrium free streaming stage, event-by-event viscous hydrodynamics, and a microscopic hadronic afterburner. Free parameters of the model, which describe the initial state and QGP medium are then simultaneously calibrated to fit charged-particle yields, mean pT, and flow cumulants. We argue that the global agreement of the calibrated model with the experimental data strongly supports the existence of hydrodynamic flow in small collision systems at ultrarelativistic energies, and that the flow produced develops at length scales smaller than a single proton. Posterior estimates for the model's input parameters are obtained, and new insights into the temperature dependence of the QGP transport coefficients and event-by-event structure of the proton are discussed.


Estimated temperature-dependent specific shear viscosity of the QGP compared with common fluids
The orange line and band show the posterior median and 90% credible region for the QGP (η∕s)(T)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\eta /s)(T)$$\end{document} estimated from Pb–Pb collision data at sNN=2.76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt {s_{{\mathrm{NN}}}} = 2.76$$\end{document} and 5.02 TeV. The blue and green lines show (η∕s)(T)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\eta /s)(T)$$\end{document} for water and helium at different pressures relative to their critical pressures, as annotated, calculated from NIST data³¹. The temperature dependence is shown relative to each fluid’s critical temperature, T/Tc.
Estimated temperature dependence of the specific shear and bulk viscosity
Left column: posterior medians and 90% credible regions for (η∕s)(T)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\eta /s)(T)$$\end{document} and (ζ∕s)(T)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\zeta /s)(T)$$\end{document} estimated from Pb–Pb collision data at sNN=2.76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt {s_{{\mathrm{NN}}}} = 2.76$$\end{document} and 5.02 TeV. Right column: one-dimensional (1D) histograms showing the marginal distributions for the indicated parameters, along with 2D density histograms showing the joint distributions between the parameters. Top row: shear viscosity; bottom row: bulk viscosity.
Posterior distribution for the initial energy deposition parameter
Top: marginal distribution for the parameter p estimated from Pb–Pb collision data at sNN=2.76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt {s_{{\mathrm{NN}}}} = 2.76$$\end{document} and 5.02 TeV, with annotations for the approximate values⁸ of other initial condition models: KLN³⁶ (p ≈ −0.67 ± 0.01), IP-Glasma³³ and EKRT⁶ (p ≈ 0.0 ± 0.1), and wounded nucleon (p = 1). Bottom: realistic initial energy density profiles in the transverse (xy) plane for a Pb–Pb collision with impact parameter b = 9 fm generated by the TRENTo model with p = −1, 0 and 1. The nucleon positions and all other aspects besides p are identical in each profile.
Model calculations using the best-fit MAP parameters compared to experimental data
Each plot shows the centrality dependence of one or more observables, as annotated. Upper left: yields of charged particles (Nch, scaled by a factor of 25 for visual clarity), transverse energy (ET, scaled by 5) and identified pions (π), kaons (K) and protons (p). Lower left: mean transverse momenta of identified pions (π), kaons (K) and protons (p). Lower right: mean transverse momentum fluctuations. Upper right: anisotropic flow cumulants vn{k} of different orders. Coloured lines are model calculations for Pb–Pb collisions at sNN=2.76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt {s_{{\mathrm{NN}}}} = 2.76$$\end{document} TeV and 5.02 TeV. Points are experimental data from ALICE21–27 for Pb–Pb collisions at sNN=2.76\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt {s_{{\mathrm{NN}}}} = 2.76$$\end{document} TeV and 5.02 TeV (some data are not available for 5.02 TeV collisions at the time of writing), where the bands denote systematic uncertainty and error bars statistical uncertainty (most error bars are too small to be seen beyond the data points). The ratio axes show the ratio of the model calculations to the data (where available), with the grey band indicating 10% deviation. The MAP parameter values, which are identical at the two energies except for the initial-condition normalization, are listed in Supplementary Table 1.
Bayesian estimation of the specific shear and bulk viscosity of quark–gluon plasma
  • Article
  • Publisher preview available

November 2019

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621 Reads

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566 Citations

Nature Physics

Ultrarelativistic collisions of heavy atomic nuclei produce an extremely hot and dense phase of matter, known as quark–gluon plasma (QGP), which behaves like a near-perfect fluid with the smallest specific shear viscosity—the ratio of the shear viscosity to the entropy density—of any known substance¹. Due to its transience (lifetime ~ 10⁻²³ s) and microscopic size (10⁻¹⁴ m), the QGP cannot be observed directly, but only through the particles it emits; however, its characteristics can be inferred by matching the output of computational collision models to experimental observations. Previous work, using viscous relativistic hydrodynamics to simulate QGP, has achieved semiquantitative constraints on key physical properties, such as its specific shear and bulk viscosity, but with large, poorly defined uncertainties2–8. Here, we present the most precise estimates so far of QGP properties, including their quantitative uncertainties. By applying established Bayesian parameter estimation methods⁹ to a dynamical collision model and a wide variety of experimental data, we extract estimates of the temperature-dependent specific shear and bulk viscosity simultaneously with related initial-condition properties. The method is extensible to other collision models and experimental data and may be used to characterize additional aspects of high-energy nuclear collisions.

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Figure 4. Transverse momentum spectra of pions, kaons and protons from p-Pb collisions at 5.02 TeV with different numbers of charged tracks in |η| < 2.4 (8 (dots), 84 (squares), 160 (triangles), 235 (inverted triangles)) as measured by CMS [26]. The lines show numerical simulations with the EPOS3.076 code which features a viscous fluid dynamic core [27]. Similar behavior was found in by CMS in p-p collisions at 0.9, 2.76 and 7 TeV [28]. Figure taken from [27].
Figure 5. Normalized shear stress π/(e+P eq ) = 1
Hydrodynamic flow in small systems or: “How the heck is it possible that a system emitting only a dozen particles can be described by fluid dynamics?”

July 2019

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100 Reads

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43 Citations

Journal of Physics Conference Series

The “unreasonable effectiveness” of relativistic fluid dynamics in describing high energy heavy-ion and even proton-proton collisions will be demonstrated and discussed. Several recent ideas of optimizing relativistic fluid dynamics for the specific challenges posed by such collisions will be presented, and some thoughts will be offered why the framework works better than originally expected. I will also address the unresolved question where exactly hydrodynamics breaks down, and why.


Initial conditions of bulk matter in ultrarelativistic nuclear collisions

April 2019

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6 Reads

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1 Citation

Dynamical models based on relativistic fluid dynamics provide a powerful tool to extract the properties of the strongly-coupled quark-gluon plasma (QGP) produced by ultrarelativistic nuclear collisions. The largest source of uncertainty in these model-to-data extractions is the choice of theoretical initial conditions (ICs) used to model the distribution of energy or entropy at the hydrodynamic starting time. Descriptions of the ICs are generally improved through iterative cycles of testing and refinement. Individual models are compared to experimental data; the worst models are discarded and best models retained. Consequently, successful traits (assumptions) are passed on to subsequent generations of the theoretical landscape. This bottom-up approach correspondingly describes a form of theoretical trial and error, where each trial proposes an ab initio solution to the problem at hand. A natural complement to this strategy, is to employ a top-down or data-driven approach which is able to reverse engineer properties of the ICs from the constraints imposed by the experimental data. In this dissertation, I motivate and develop a parametric IC model based on a family of functions known as the generalized means. The ansatz closely mimics the variability of ab initio calculations and serves as a reasonable parametric form for exploring QGP energy and entropy deposition assuming imperfect knowledge of the complex physical processes which lead to its creation. With the parametric model in hand, I explore broad implications of the proposed ansatz using recently adapted Bayesian methods to simultaneously constrain properties of the ICs and QGP medium using experimental data from the Large Hadron Collider. These analyses show that the ICs are highly constrained by available measurements and provide evidence of a unified hydrodynamic description of small and large nuclear collision systems.


Hydrodynamic flow in small systems, or: "How the heck is it possible that a system emitting only a dozen particles can be described by fluid dynamics?"

April 2019

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26 Reads

The "unreasonable effectiveness" of relativistic fluid dynamics in describing high energy heavy-ion and even proton-proton collisions are demonstrated and discussed. Several recent ideas of optimizing relativistic fluid dynamics for the specific challenges posed by such collisions will be presented, and some thoughts will be offered why the framework works better than originally expected. I will also address the unresolved question where exactly hydrodynamics breaks down, and why.


Fig. 1. Left-side: computed observables at each design point. Right-side: posterior samples from the calibrated emulator.
Fig. 2. Joint posterior probability distribution for the nucleon width w and the constituent width v. The gray shaded region v > w is excluded by the chosen prior.
Fig. 3. Posterior 90% credible regions for the temperature dependent shear viscosity (left) and temperature dependent bulk viscosity (right) from the present combined p-Pb and Pb-Pb analysis at √ s NN = 5.02 TeV (orange hatch), compared to a previous Bayesian analysis of Pb-Pb collisions at √ s NN = 2.76 and 5.02 TeV (blue band) [5].
Estimating nucleon substructure properties in a unified model of p-Pb and Pb-Pb collisions

February 2019

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122 Reads

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8 Citations

Nuclear Physics A

We apply a well tested hybrid transport model, which couples viscous hydrodynamics to a hadronic afterburner, to describe bulk observables in proton-lead and lead-lead collisions at sNN=5.02TeV. The quark-gluon plasma (QGP) initial conditions are modeled using the parametric TRENTo model with additional nucleon substructure parameters to vary the number and size of hot spots inside each nucleon, followed by a pre-equilibrium free streaming stage to match the full energy-momentum tensor of the initial state onto viscous hydrodynamics. Initial condition and QGP medium parameters, such as the temperature dependence of the QGP shear and bulk viscosities, are then calibrated using Bayesian parameter estimation to describe charged particle yields, mean pT and anisotropic flow harmonics of both collision systems in a single self-consistent framework. We find that the hybrid model provides a compelling, simultaneous description of both collision systems using appropriately chosen model parameters, and present new posterior estimates for the size and shape of the nucleon and temperature dependence of QGP shear and bulk viscosities.


Estimating initial state and quark-gluon plasma medium properties using a hybrid model with nucleon substructure calibrated to p-Pb and Pb-Pb collisions at sNN=5.02\sqrt{s_\mathrm{NN}}=5.02 TeV

August 2018

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10 Reads

We posit a unified hydrodynamic and microscopic description of the quark-gluon plasma (QGP) produced in ultrarelativistic p-Pb and Pb-Pb collisions at sNN=5.02\sqrt{s_\mathrm{NN}}=5.02 TeV and evaluate our assertion using Bayesian inference. Specifically, we model the dynamics of both collision systems using initial conditions with parametric nucleon substructure, a pre-equilibrium free-streaming stage, event-by-event viscous hydrodynamics, and a microscopic hadronic afterburner. Free parameters of the model which describe the initial state and QGP medium are then simultaneously calibrated to fit charged particle yields, mean pTp_T, and flow cumulants. We argue that the global agreement of the calibrated model with the experimental data strongly supports the existence of hydrodynamic flow in small collision systems at ultrarelativistic energies, and that the flow produced develops at length scales smaller than a single proton. Posterior estimates for the model's input parameters are obtained, and new insights into the temperature dependence of the QGP transport coefficients and event-by-event structure of the proton are discussed.


Estimating nucleon substructure properties in a unified model of p-Pb and Pb-Pb collisions

June 2018

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12 Reads

We apply a well tested hybrid transport model, which couples viscous hydrodynamics to a hadronic afterburner, to describe bulk observables in proton-lead and lead-lead collisions at sNN=5.02\sqrt{s_{NN}}=5.02 TeV. The quark-gluon plasma (QGP) initial conditions are modeled using the parametric TRENTO model with additional nucleon substructure parameters to vary the number and size of hot spots inside each nucleon, followed by a pre-equilibrium free streaming stage to match the full energy-momentum tensor of the initial state onto viscous hydrodynamics. Initial condition and QGP medium parameters, such as the temperature dependence of the QGP shear and bulk viscosities, are then calibrated using Bayesian parameter estimation to describe charged particle yields, mean pTp_T and anisotropic flow harmonics of both collision systems in a single self-consistent framework. We find that the hybrid model provides a compelling, simultaneous description of both collision systems using appropriately chosen model parameters, and present new posterior estimates for the size and shape of the nucleon and temperature dependence of QGP shear and bulk viscosities.


Constraints on rapidity-dependent initial conditions from charged particle pseudorapidity densities and correlations at the LHC

August 2017

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12 Reads

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3 Citations

Nuclear and Particle Physics Proceedings

The initial three-dimensional entropy distribution of the quark-gluon plasma produced in relativistic heavy-ion collision is systematically studied using parametric initial conditions. We apply a cumulant generating function approach to parametrize the rapidity dependence of local entropy deposition and extend the boost-invariant initial condition model TRENTo to include longitudinal structure. Two different parametrizations are tested and their parameters optimized by comparing to centrality dependent charged particle pseudorapidity densities of p+Pb (5.02A TeV) and Pb+Pb (2.76A TeV) using Bayesian inference. Successful parametrizations are then selected based on their ability to describe two-particle psuedorapidity correlations. Finally, we predict the pseudorapidity dependent flows and event-plane decorrelations using the optimized initial conditions and a 3+1D hybrid hydro+micro model.


Determination of Quark-Gluon-Plasma Parameters from a Global Bayesian Analysis

April 2017

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2 Reads

The quality of data taken at RHIC and LHC as well as the success and sophistication of computational models for the description of ultra-relativistic heavy-ion collisions have advanced to a level that allows for the quantitative extraction of the transport properties of the Quark-Gluon-Plasma. However, the complexity of this task as well as the computational effort associated with it can only be overcome by developing novel methodologies: in this paper we outline such an analysis based on Bayesian Statistics and systematically compare an event-by-event heavy-ion collision model to data from the Large Hadron Collider. We simultaneously probe multiple model parameters including fundamental quark-gluon plasma properties such as the temperature-dependence of the specific shear viscosity η/s\eta/s, calibrate the model to optimally reproduce experimental data, and extract quantitative constraints for all parameters simultaneously. The method is universal and easily extensible to other data and collision models.


Citations (18)


... More information can be obtained from the detailed analysis of the results of transport approaches, which describe the time evolution of the QGP. Employing the technique of Bayesian analysis constraints on the shape of the initial state, shear [8] and bulk [9] viscosity of the QGP medium and its equation of state [10] can be established. ...

Reference:

SUBA-jet: a new model for jets in heavy ion collisions
Applying Bayesian parameter estimation to relativistic heavy-ion collisions: simultaneous characterization of the initial state and quark-gluon plasma medium
  • Citing Preprint
  • May 2016

Jonah E. Bernhard

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J. Scott Moreland

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Steffen A. Bass

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[...]

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Ulrich Heinz

... Specifically, an event of a heavy-ion collision, from the time of collision until the detection of particles, passes through a number of successive stages [25,27,28]. At the time of the collision, the colliding nuclei deposit energy or entropy at the overlap region, which serves as the initial state or initial condition of the collision. ...

Bayesian calibration of a hybrid nuclear collision model using p − Pb and Pb-Pb data at energies available at the CERN Large Hadron Collider
  • Citing Article
  • February 2020

Physical Review C

... The QGP formed in a collision undergoes a quick phase of thermalization [8] before it expands as a relativistic hydrodynamic fluid. The hydrodynamic description of the QGP stands as one of the great successes in developing an effective theory of many-body quantum chromodynamics (QCD) at high temperatures [6,9,10]. As the system expands, both its energy and entropy density decrease and eventually the system undergoes a phase transition as a consequence of which hadrons are formed [11,12]. ...

Bayesian estimation of the specific shear and bulk viscosity of quark–gluon plasma

Nature Physics

... The collective behavior observed in small systems can be interpreted through various approaches. Prominent explanations include initial-state correlations [46], partonic scattering and the formation of color flux tubes [47], and hydrodynamic flow [48]. An alternative framework for describing such collective flow is kinetic theory. ...

Hydrodynamic flow in small systems or: “How the heck is it possible that a system emitting only a dozen particles can be described by fluid dynamics?”

Journal of Physics Conference Series

... 1 From analytical Glauber model, the probability of n nucleonnucleon collision is calculated using the single nucleon-nucleon collision probability, P coll nn (bn) of Eq. (8). And using that, one can find the average number of nucleons that participate in more than one pairwise collisions (N A part and N B part ) from each nucleus A and B [41] Here, N A part is the number of participating nucleons from nucleus A, b is the nucleus-nucleus collision impact parameter and γ i is a weight factor sampled from a gamma distribution to introduce fluctuations like that in between events in the experimental setup [42]. An analogous equation is used for nucleus B with a negative sign for b/2 term. ...

Initial conditions of bulk matter in ultrarelativistic nuclear collisions
  • Citing Preprint
  • April 2019

... As such systems were in principle not expected to exhibit collective effects, these measurements opened up an intense discussion on whether the observed flow originates from momentum correlations intrinsic to the colliding objects or from the final state response to the initial geometry of the system. Regarding the contribution that arises from initial geometry, multiple studies [8][9][10][11][12][13][14] suggest that the event-by-event fluctuation of subnucleonic degrees of freedom plays an essential role in the emergence of correlations in small systems. The description of such fluctuations relies heavily on phenomenological models, which include, e.g., randomly changing partonic structures and/or quantum fluctuations of color charge densities. ...

Estimating nucleon substructure properties in a unified model of p-Pb and Pb-Pb collisions

Nuclear Physics A

... The procedure will follow that described in Refs. [33,211,216,[351][352][353][354][355][356][357][358][359][360][361]. Those analyses provide a sampling of the model parameters weighted by the posterior Bayesian likelihood. ...

Constraints on rapidity-dependent initial conditions from charged particle pseudorapidity densities and correlations at the LHC
  • Citing Article
  • August 2017

Nuclear and Particle Physics Proceedings

... In practice, this can be achieved only by performing a fluid-dynamics based "global analysis," a simultaneous study of various different (low-transversemomentum) observables from as many types of collision systems as possible. These analyses have evolved from pioneering works [12,14,17] (see also [22]) to those with a proper Bayesian statistical analysis and well defined uncertainty estimates [21,[23][24][25][26][27][28][29][30][31]. So far, the analyses have mainly focused on studies at midrapidity, where one assumes a longitudinally boost symmetric (but three-dimensionally expanding) system described by the (2 + 1)D fluid dynamical equations of motion. ...

Determination of Quark-Gluon-Plasma Parameters from a Global Bayesian Analysis

Nuclear Physics A

... Such a model can then produce predictions for many different observables for each particular set of input parameters. By using such a model in a Bayesian analysis, it is then possible to fit the input parameters to real experimental data, allowing one to learn something about which input parameters fit the data best [196][197][198][199][200][201][202][203][204]. ...

Flow in small and large quark-gluon plasma droplets: the role of nucleon substructure
  • Citing Article
  • April 2017

Nuclear Physics A

... It does this by mapping inputs to outputs and learning the functional relationship between them rather than attempting to produce a coarse version of the intermediary physics. These methods have had success in heavy ion physics [25,[28][29][30][31][39][40][41][42][43][44]. ...

Characterization of the initial state and QGP medium from a combined Bayesian analysis of LHC data at 2.76 and 5.02 TeV

Nuclear Physics A