“…2). In solid helium the target exposed to the high power laser radiation heats up and melts the helium crystal in a nearby volume of several mm 3 (Fig. 1).…”
“…Liquid 4 He is a peculiar solvent because of its low temperature, exceptionally low electric polarizability, large heat conductivity, high purity and chemical inertness. In particular the heat conductivity of liquid helium above T = 2.17 K (He I) is ≈0.02 W/m·K (compare to 0.58 W/m·K for water or 0.17 W/m·K for ethanol at room temperature), whereas in the superfluid helium (He II) below T = 2.17 K the heat flow becomes nonlinear function of the temperature gradient and is several orders of magnitude higher than in He I [3]. Viscosity of He I is ≈2 × 10 −6 Pa·s (that is three orders of magnitude smaller than that of water at room temperature) and vanishes in He II.…”
Laser ablation of metals in liquid helium results in the formation of metal filaments with diameters on the order of 2-10 nanometres and of spherical nanoparticles. In superfluid helium these nanowires aggregate into centimeter-sized networks. We study the morphology and the electric conductivity of these large aggregates, as well as extinction spectra and the crystalline structure of the individual nanofragments. We discuss the effect of superfluidity on the mechanisms of coalescence processes at the nanometer and centimeter scales.
“…2). In solid helium the target exposed to the high power laser radiation heats up and melts the helium crystal in a nearby volume of several mm 3 (Fig. 1).…”
“…Liquid 4 He is a peculiar solvent because of its low temperature, exceptionally low electric polarizability, large heat conductivity, high purity and chemical inertness. In particular the heat conductivity of liquid helium above T = 2.17 K (He I) is ≈0.02 W/m·K (compare to 0.58 W/m·K for water or 0.17 W/m·K for ethanol at room temperature), whereas in the superfluid helium (He II) below T = 2.17 K the heat flow becomes nonlinear function of the temperature gradient and is several orders of magnitude higher than in He I [3]. Viscosity of He I is ≈2 × 10 −6 Pa·s (that is three orders of magnitude smaller than that of water at room temperature) and vanishes in He II.…”
Laser ablation of metals in liquid helium results in the formation of metal filaments with diameters on the order of 2-10 nanometres and of spherical nanoparticles. In superfluid helium these nanowires aggregate into centimeter-sized networks. We study the morphology and the electric conductivity of these large aggregates, as well as extinction spectra and the crystalline structure of the individual nanofragments. We discuss the effect of superfluidity on the mechanisms of coalescence processes at the nanometer and centimeter scales.
“…Here we give a brief introduction to the problem of heat transport along thin tubes, which is in fact one of the most challenging topics in heat transfer [81,83,84].…”
Section: Thin Tubes Filled With Superfluid Heliummentioning
We provide an overview on the problem of modeling heat transport at nanoscale and in far-from-equilibrium processes. A survey of recent results is summarized, and a conceptual discussion of them in the framework of Extended Irreversible Thermodynamics is developed.
“…Since there are numerous cryopumps in the spectrometer, one must consider the effects on the boiling point of changing the nuclear mass in helium from 4 to 65 u. This is described in detail by Wilks [19], who gives the procedure for determining the boiling point for 65 He; we calculated it to be 7 K. Thus the cryopumps in the system, which operate at a variety of temperatures, but always above 10 K, should not affect the strangelet to 4 He abundance ratio.…”
Section: B Enhancement Of Measured Abundance Limitsmentioning
A search for stable strange quark nuggets has been conducted in helium and argon using a high sensitivity mass spectrometer. The search was guided by a mass formula for strange quark nuggets which suggested that stable strange helium might exist at a mass around 65 u. The chemical similarity of such "strangelets" to noble gas atoms and the gravitational unboundedness of normal helium result in a large enhancement in the sensitivity of such a search. An abundance limit of no more than 2 · 10 −11 strangelets per normal nucleus is imposed by our search over a mass region from 42 to 82 u, with much more stringent limits at most (non-integer) masses.
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