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FR06 · Conditional Bayesian inference

QGP Transport Inference

How much does a viscosity estimate depend on the initial state? A viscosity estimate depends on the initial geometry and on correlations that do not come from collective flow. The same saved synthetic events give different conditional posteriors when those assumptions change, so a narrow interval alone cannot establish an unconditional QGP viscosity.

Fit one fixed synthetic event sample under different initial geometries and pair backgrounds. Watch the viscosity posterior move and widen as the assumptions change.

Interactive modelQGP Transport Inference

Reading the fixed synthetic event sample.

Model, units and sources

Natural units are used. The Gaussian density has unit mean squared radius per axis before deformation. Its short-axis direction defines the elliptic emission plane. This is an assigned response calculation, with no transverse fluid solver.

vn=κ0εne−1.8n2(η/s)/(RT),n=2,3v_n=\kappa_0\varepsilon_n e^{-1.8n^2(\eta/s)/(RT)},\qquad n=2,3

The response coefficient and damping scale are illustrative. Higher harmonics and nonlinear mode coupling are omitted.

Gardim et al. (2012) · Bilandzic et al. (2011) · Bernhard et al. (2019)

Physics tutorial

QGP Transport Inference

BackgroundFit one fixed synthetic event sample under different initial geometries and pair backgrounds. Watch the viscosity posterior move and widen as the assumptions change.

Why it mattersA finite-lived cloud leaves particle directions behind. Inferring its viscosity requires a prediction of how its unknown initial shape becomes those directions.

Start with the essentials

Focus question
How much does a viscosity estimate depend on the initial state?
One-sentence intuition
The same particle correlations can favor different viscosities when the initial geometry or pair background changes.

Core mathematical model

Distinct-particle pair correlation

Cn=∣Qn∣2−MM(M−1),Qn=∑j=1MeinϕjC_n=\frac{|Q_n|^2-M}{M(M-1)},\qquad Q_n=\sum_{j=1}^{M}e^{in\phi_j}

Subtracting multiplicity removes each particle paired with itself. The saved event flow vectors determine every plotted correlation.

Four-particle cumulant

cn{4}=⟨⟨4⟩⟩−2⟨⟨2⟩⟩2c_n\{4\}=\langle\langle4\rangle\rangle-2\langle\langle2\rangle\rangle^2

Four distinct particles contribute to each four-particle term. Cumulants suppress many pair backgrounds; finite samples and clusters that themselves flow still matter.

Conditional posterior

p(η/s,κ0∣D,M)∝exp⁡ ⁣[−12ΔTΣ−1Δ]p(η/s,κ0)p(\eta/s,\kappa_0\mid D,\mathcal M)\propto\exp\!\left[-\tfrac12\Delta^\mathsf T\Sigma^{-1}\Delta\right]p(\eta/s,\kappa_0)

The residual compares the same six observed pair means with the selected model. Marginalizing the response amplitude gives the viscosity interval.

Common difficulties

What the estimate means

Typical misconceptionA narrow posterior fixes the viscosity of real QGP.

Better mental modelThe displayed interval conditions on the chosen response, geometry, priors, and error model. Real extractions also simulate the full collision and compare many observables.

Run the experiment

  1. 01

    Keep the sample fixed

    Start with Planted assumptions, then download the event records.

    What to observe: The benchmark holds 4,500 events. Its seed and generation parameters travel with the records.
  2. 02

    Change the initial geometry

    Choose Larger ellipticity and compare the shaded interval.

    What to observe: The data points stay put. The model and conditional posterior move.
  3. 03

    Test the background

    Choose Ignore doublets, then Allow model error.

    What to observe: A background change shifts the estimate; a larger discrepancy generally broadens the range compatible with the same sample.

Related experiments and articles

Heavy-ion matter and hydrodynamics · Reading path

From directional pressure to transport inference

Articles on this path that use this experiment, followed by the other experiments they suggest.

  1. ArticleMeasure common flow through particle correlations
  2. ArticleInfer transport while changing the assumed initial state
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