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81.
82.
83.
G. E. Volovik 《Journal of Low Temperature Physics》2008,150(3-4):453-463
Superfluid 3He-A shares the properties of spin nematic and chiral orbital ferromagnet. Its order parameter is characterized by two vectors
and
. This doubly anisotropic superfluid, when it is confined in aerogel, represents the most interesting example of a system
with continuous symmetry in the presence of random anisotropy disorder. We discuss the Larkin-Imry-Ma state, which is characterized
by the short-range orientational order of the vector
, while the long-range orientational order is destroyed by the collective action of the randomly oriented aerogel strings.
On the other hand, sufficiently large regular anisotropy produced either by the deformation of the aerogel or by applied superflow
suppresses the Larkin-Imry-Ma effect leading to the uniform orientation of
. The interplay of regular and random anisotropy allows us to study many different effects.
相似文献
84.
I. A. Fomin 《Journal of Low Temperature Physics》2008,150(3-4):464-471
A mutual action of the random anisotropy brought in the superfluid 3He by aerogel and of the global anisotropy caused by its deformation is considered. Strong global anisotropy tends to suppress
fluctuations of orientation of the order parameter and stabilizes ABM order parameter. In a limit of vanishing anisotropy
fluctuations of ABM order parameter became critical. It is argued that still in a region of small fluctuations the order parameter
changes its form to be less sensitive to the random anisotropy. For a favorable landscape of the free energy of superfluid
3He the fluctuations remain small even in a limit of vanishing global anisotropy and the long-range order is maintained.
相似文献
85.
The simplest example of fingering occurs when a heavier liquid occupies the half-space above a lighter one. The fingers of
the heavier liquid driven by gravity grow down, displacing the lighter liquid upward. The fingering of the superfluid phase
into the 4He crystal facet below its roughening transition temperature can provide us an example of macroscopic quantum nucleation phenomena.
Due to cusp-like singularity in the surface tension as a function of the facet orientation the crystal facet has a relative
stability and its fingering is accompanied by overcoming some critical nucleation barrier. The barrier height is proportional
to the square of the facet step energy and depends on a ratio of the facet size to the capillary length. At sufficiently low
temperatures the thermal activation mechanism for the interface fingering is replaced with the quantum one associated with
the penetration through the nucleation barrier.
相似文献
86.
L. LavagninoR. Moroni F. Bisio S. TerreniL. Mattera M. Canepa 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2011,269(9):932-935
We report first results on the deposition of l-cysteine (Cys), a fundamental amino-acid, on a magnetic substrate. Molecules have been deposited under ultra-high vacuum conditions on Fe(1 0 0) films. Electronic and magnetic properties of adsorbed molecules have been investigated by spin polarized metastable deexcitation spectroscopy (SPMDS). The spectra show a growth dynamics apparently similar to the one already reported on coinage metal surfaces with the formation of a strongly-bound thiolate species (SFe bond) and weakly-bound second-layer molecules. SPMDS revealed the spin-polarized character of an Auger (Penning) deexcitation peak related to a Cys molecular orbital. Interestingly, these spin-polarization effects, ascribed to the interaction with the magnetized substrate, vanish before the first layer completion, suggesting a possible correlation with the SAM assembly properties. 相似文献
87.
88.
In this paper, a mechanism about the variability of the L-H transition power thresh- old PL-H is proposed which is based on the ion orbit losses. Only in the edge where there are enough ion orbit losses and the negative radial electric field Er is high enough can the H-mode be triggered. The ion orbit losses are determined by the ion in the loss region under certain edge conditions. For different mass A and different charge Z, the critical loss energy E Z2/A in the loss region. In H and D charges, because the D+ loss region is larger than H+, it can be deduced that the PL-H of H is larger than that of D. In a 4He discharge, experiment finds there exist a considerable number of 4He1+ in the plasma edge. The actual ion orbit losses are determined by the mixing ratio of a He1+ and 4He2+. The 4He1+ loss region is larger than that of 4He2+, and the loss region of D+ interposes between 4He1+ and 4He2+. Different 4He1+ content can cause the edge ion losses in a 4He discharge to be greater than, less than or equal to that in a D discharge. So a 4He discharge can exhibit multiple experimental phenomena in the PL-H. 相似文献
89.
文章描述了磷灰石(U-Th)/He热年代学方法的基本测年原理、校正模型、封闭温度和实践验证,及此方法在古地形演化、山体剥露历史和剥蚀速率研究中的应用。 相似文献
90.