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We are focusing on the crystallization of 4 He in aerogels intensively, motivated by the finding of the dynamical transition of the crystal growth inside the aerogels. 1 In the experiment with aerogels contained in a flat glass tube, we found that 4 He in the aerogel crystallized by nucleation. 2 In order to confirm this nucleation, we measured the critical overpressure at which the very first 4 He crystal appears in the aerogel. Crystallization and melting were repeated 50 times at a constant temperature in a variable volume cell and the nucleation probability as a function of overpressure was obtained. Anisotropic S shape characteristic to the nucleation process was successfully observed and the critical radius of the nucleated crystals was estimated. The S shape curve changes drastically through the dynamical transition temperature.

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The phase boundary between the quantum solid and liquid phases of 4 He is strongly modified in a porous material. However the phase diagram at very low temperatures remains unexplored. We have used a variable-volume experimental cell with optical access to visualize the crystallization of 4 He in silica aerogels with independent control of the pressure and temperature. The onset of crystallization was investigated in two aerogel samples with differing porosity both by pressurization at constant temperature and by cooling at constant pressure. With isothermal pressurization we have established a low temperature phase diagram for each aerogel and we find that the equilibrium crystallization pressure is reduced with increasing aerogel porosity. Crystals also began to grow in the aerogel on cooling at fixed pressure below an onset temperature, Tgrow. We found that below this temperature the crystallization rate increased with decreasing temperature. The aerogel in our cell was surrounded by bulk crystals of 4 He and surprisingly Tgrow was found to be widely distributed when the surrounding bulk crystals were repressurized. In this experimental arrangement, crystallization within the aerogel on cooling requires mass flow from these exterior bulk crystals and is strongly influenced by the disordered structure at the interface between the bulk solid and the helium within the aerogel.