Self-consistent measurement of the equation of state of liquid deuterium

2012 ◽  
Vol 8 (1) ◽  
pp. 76-80 ◽  
Author(s):  
K. Falk ◽  
S.P. Regan ◽  
J. Vorberger ◽  
M.A. Barrios ◽  
T.R. Boehly ◽  
...  
1981 ◽  
Vol 24 (2) ◽  
pp. 724-729 ◽  
Author(s):  
K. Shukla ◽  
A. Paskin ◽  
D. O. Welch ◽  
G. J. Dienes

1982 ◽  
Vol 25 (2) ◽  
pp. 1297-1309 ◽  
Author(s):  
A. Paskin ◽  
A. -M. Llois de Kreiner ◽  
K. Shukla ◽  
D. O. Welch ◽  
G. J. Dienes

1993 ◽  
Vol 137 ◽  
pp. 307-309 ◽  
Author(s):  
D. Saumon ◽  
G. Chabrier

An improved theory of fluid hydrogen at high density, based on a detailed treatment of inter-particle correlations and a self-consistent treatment of pressure ionization, has become available recently (Chabrier 1990, Saumon and Chabrier 1991, 1992). We present a preliminary comparison between this new EOS (hereatfer SC) and equations of state frequently used in astrophysical contexts, namely: Fontaine, Graboske and Van Horn 1977 (FGVH), Däppen et al. 1988 (MHD) and Magni and Mazzitelli 1979 (MM).The SC theory predicts a first-order phase transition in the region of pressure-ionization (the so-called Plasma Phase Transition, or PPT), between an essentially neutral mixture of atoms and molecules (xe– < 10−2), and a partially ionized plasma (xe– ≈ 50 %), with a critical point located at Pc = 0.614 Mbar, Tc = 15300K and pc = 0.35 g/cm3.


2012 ◽  
Vol 18 ◽  
pp. 216-220
Author(s):  
J. PERALTA-RAMOS ◽  
M. S. NAKWACKI

We use a self-consistent chiral-hydrodynamic formalism which combines the linear σ model with second-order hydrodynamics in 2 + 1 dimensions to compute the spectrum of thermal photons produced in Au+Au collisions at [Formula: see text]. The temperature-dependent shear viscosity of the model, η, is calculated from the linearized Boltzmann equation. We compare the results obtained in the chiral-hydrodynamic model to those obtained in the second-order theory with a Lattice QCD equation of state and a temperature-independent value of η/s. We find that the thermal photon production is significantly larger in the latter model due to a slower evolution and larger dissipative effects.


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