2011
DOI: 10.1103/physreve.83.051507
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Droplet evolution in expanding flow of warm dense matter

Abstract: We propose a simple, self-consistent kinetic model for the evolution of a mixture of droplets and vapor expanding adiabatically in vacuum after rapid, almost isochoric heating. We study the evolution of the two-phase fluid at intermediate times between the molecular and the hydrodynamic scales, focussing on out-of-equilibrium and surface effects. We use the Van der Waals equation of state as a test-bed to implement our model and study the phenomenology of the upcoming NDCXII ion heating experiments at LBNL. We… Show more

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Cited by 15 publications
(20 citation statements)
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“…These Bose-Einstein condensates have been studied both at finite size and in the thermodynamic limit focusing on mathematical structures and general properties (Beau and Zagrebnov, 2010;van den Berg, 1983;van den Berg and Lewis, 1982;van den Berg et al, 1986a,b;Casimir, 1968;van Druten and Ketterle, 1982;Girardeau, 1960Girardeau, , 1965Ketterle and van Druten, 1982;Krueger, 1968;Mullin, 1997;Mullin and Sakhel, 2012;Rehr, 1970;Zobay and Garraway, 2004), in connection with liquid helium in thin films (Douglass et al, 1964;Goble and Trainor, 1965, 1966, 1967Khorana and Douglass, 1965;Mills, 1964;Osborne, 1949), magnetic flux of superconducting rings (Sonin, 1969), and gravito-optical traps (Wallis, 1996). Experimental realizations of effective low dimensional Bose-Einstein condensates with trapped atoms have been reported in (van Amerongen, 2008;van Amerongen et al, 2008;Armijo et al, 2011;Bouchoule et al, 2011;Esteve et al, 2006;Görlitz et al, 2001;Greiner et al, 2001). I µ,µ in these Bose-Einstein condensate phases is superextensive and interpolates between the scaling above the critical temperature and I µ,µ = O β 2 N 2 for a standard Bose-Einstein condensate only consisting of the ground state.…”
Section: Role Of Quantum Statisticsmentioning
confidence: 99%
“…These Bose-Einstein condensates have been studied both at finite size and in the thermodynamic limit focusing on mathematical structures and general properties (Beau and Zagrebnov, 2010;van den Berg, 1983;van den Berg and Lewis, 1982;van den Berg et al, 1986a,b;Casimir, 1968;van Druten and Ketterle, 1982;Girardeau, 1960Girardeau, , 1965Ketterle and van Druten, 1982;Krueger, 1968;Mullin, 1997;Mullin and Sakhel, 2012;Rehr, 1970;Zobay and Garraway, 2004), in connection with liquid helium in thin films (Douglass et al, 1964;Goble and Trainor, 1965, 1966, 1967Khorana and Douglass, 1965;Mills, 1964;Osborne, 1949), magnetic flux of superconducting rings (Sonin, 1969), and gravito-optical traps (Wallis, 1996). Experimental realizations of effective low dimensional Bose-Einstein condensates with trapped atoms have been reported in (van Amerongen, 2008;van Amerongen et al, 2008;Armijo et al, 2011;Bouchoule et al, 2011;Esteve et al, 2006;Görlitz et al, 2001;Greiner et al, 2001). I µ,µ in these Bose-Einstein condensate phases is superextensive and interpolates between the scaling above the critical temperature and I µ,µ = O β 2 N 2 for a standard Bose-Einstein condensate only consisting of the ground state.…”
Section: Role Of Quantum Statisticsmentioning
confidence: 99%
“…In this paper, in a similar manner to previous studies (Barnard et al, 2007;Armijo & Barnard, 2011), we propose a simple, safe, and inexpensive experimental setup, where a small amount of fissile sample is almost homogeneously and instantaneously heated by an intense short-pulsed medium-energy heavy-ion beam. For precise assessment of high-pressure EOS of fissile materials, subsequent hydrodynamic motion is examined in detail.…”
Section: Introductionmentioning
confidence: 99%
“…Experimentally, we prepare clouds of 87 Rb atoms by radio-frequency evaporation in our atom-chip experiment, as described in [26], and we record a set of density profiles taken under the same experimental conditions. The longitudinal trapping frequency is 6.2 Hz, while the transverse confinement is 1.9 kHz.…”
mentioning
confidence: 99%
“…Since the local density approximation is well fulfilled longitudinally, the equilibrium profile can be computed using the equation of state for longitudinally homogeneous gases, ρ(µ, T ), where µ is the chemical potential. Using the well-established modified Yang-Yang equation of state [26,27], where the effective 1D coupling constant is g = 2 ω ⊥ a, the experimental density profile is fitted for a temperature T pr = 140 nK (see Fig. 4).…”
mentioning
confidence: 99%
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