Page 1
Overview Results Looking Forward
FRIB Experiments: Equation of StatePawel Danielewicz (MSU)
Goals f/Central ReactionResearch:• Characteristics of
Nuclear Matter• Reaction Mechanisms• Methods (Transport,
Observables)Kim JKPS71(17)628
1 2 3 4 5!/!
0
1
10
100
P (M
eV/fm
3 )
Danielewicz et alNL3FSUIU-FSU
Symmetric Matter
Fattoyev PRC82(10)055803
Matter Characteristics:– Equations of State– Optical Potentials– Transport Coefficients– Process Rates
Page 2
Overview Results Looking Forward
Reaction Mechanisms• Compression Stage
(Equilibration, Generation ofFlows, Meson Production)• From Compression to Final
Stage (FragmentProduction, Instabilities)
Colonna PPNP, in press
Lin arXiv:1912.11069
Methods– Transport
(Semiclassical/Quantum,Accuracy, Fluctuations)
– Observables f/MultiparticleFinal States
– Impact on Detectors– Machine Learning,
Uncertainty Quantification
Page 3
Overview Results Looking Forward
Equation of State
EA (ρ, δ,T )⇒ E
A (ρ, δ = 0,T = 0)
P(ρ, δ,T ) – fundamental relation
δ = (ρn − ρp)/ρ – asymmetry
Observables• Flow• Subthreshold K Yields
0 1 2 3 4 5ρ/ρ0
100
101
102
103
P [M
eV fm
-3]
KaoS exp. Flow dataBHF, Av 18 + UVIX TBF
BHF, Av 18 + micro TBF
BHF, Bonn B + micro TBFAPR, Av 18 + UVIX TBFDBHF
Symmetric nuclear matter
Baldo PPNP91(16)203
Lynch
Page 4
Overview Results Looking Forward
Transport Coefficients
Shear Viscosityη(ρ, δ = 0,T )
Observables: StoppingBarker PRC99(19)034607
0
20
40
60
80
100
120
140
10 30 50 70
η[M
eV/fm
2c]
T (MeV)
ρ/ρ0 = 0 .5
10 30 50 70
T (MeV)
ρ/ρ0 = 1
10 30 50 70
T (MeV)
ρ/ρ0 = 2
ν = 0 .4ν = 0 .6ν = 0 .8Fuchs
Rostockfree
Realistic Bundle
Shear Viscosity
Page 5
Overview Results Looking Forward
Isoscalar Optical PotentialObservable: p⊥ Dependence of Elliptic Anisotropy at y = 0
RN =N(−90◦) + N(90◦)N(0◦) + N(180◦)
PD NPA673(00)375
Page 6
Overview Results Looking Forward
Symmetry EnergyEA(ρn, ρp) =
E0
A(ρ) + S(ρ) δ2 +O(δ4)
symmetric matter (a)symmetry energy
Observables: Systematics of changes w/isospin, mirror pairs
n/Z=1 Elliptic-Flow Ratio
0.3 0.4 0.5 0.6 0.70.40.50.60.70.80.9
11.11.21.3
/A (GeV/c)t
p
ch 2/vn 2v
sti�
soft
0.10±=0.75γ
0
20
40
60
80
0 0.5 1 1.5 2
ρ/ρ0
S (M
eV)
n/ch �owBrownZhangHIC Sn+SnIASFOPI-LANDASY-EOS
Russotto PRC94(16)034608, Au+Au 400MeV/u
Page 7
Overview Results Looking Forward
Isovector Optical PotentialRelation between masses m∗n and m∗p in a n-rich system?
Data
SLy4
Skm*
��∗ � ��
∗
��∗ � ��
∗
124 124
112 112
Sn Sn
Sn Sn
E / A 120 MeV
Central Collisions
+
+=
Coupland PRC94(16)011601
Page 8
Overview Results Looking Forward
Interface w/Astrophysics
Symmetry pressure from difference between GW170817inference and δ = 0 matter from central collisions
Tsang PLB795(19)533
Page 9
Overview Results Looking Forward
Transport Code Comparison
Correlation: Major PhysicsInputs
Observables
SecondaryPhysics Inputs
TechnicalDecisions
Same major inputs, test outputs for stringent/more open-endedconditions, between codes and against known limits
Outcomes:• Collisions in closed box→
Understood• Finite system→ Some Struggle• Subthreshold π in finite system→ Mystery
Ono PRC100(19)044617Detailed Balance Test
from
exp
ecte
d
Page 10
Overview Results Looking Forward
Outlook
FRIB: Wider variation of δ f/given A or Z
Statistics: High needed to fish out centrality & quantifyreaction-plane effects, especially differential
Different nuclides could be lumped, but then these more rarewould be dominated by those more common.
Observables: Mirror products, n/p, t/3He, π−/π+
yields, spectra, flows, correlations
Physics: Isovector physics at finite ρ; finite T ; interfacew/astrophysics; dynamic instabilities; quantum transport