For instance, Sorrell (1995a,b) proposed a mechanism of grain spin-up due to interaction with cosmic rays that locally heat grains and provide evaporation of adsorbed H2 molecules.
Physics of Grain Alignment
Notice, however, that massless open string vertices in NCOS are associated only with quantum ﬂuctuations of the center-of-mass dynamics of the D1-brane (and the N adsorbed F-strings), which under T-duality becomes the IIA D0-brane.
IIA/B, Wound and Wrapped
When a dimer desorbs or adsorbs, the surface heights at two nearest neighbor sites change by one unit simultaneously.
Anomalous Roughness, Localization, and Globally Constrained Random Walks
Order-disorder transitions of adsorbed atomic layers are known to belong to different two-dimensional universality classes depending on the type of superstructures in the ordered phase of the adlayer [34, 35].
Quenched bond dilution in two-dimensional Potts models
The same experiments were then reproduced in the presence of intentionally added oxygen impurities, at a temperature which is above the ordering temperature of pure oxygen adsorbed on the same substrate.
Quenched bond dilution in two-dimensional Potts models
For this it will be important to measure the free energy as a function of the distance from an adsorbing interface.
Coil-Globule Transition for Regular, Random and Specially Designed Copolymers: Monte Carlo Simulation and Self-Consistent Field Theory
Superﬂuid 4He adsorbed in Vycor glass can be modeled by a three-dimensional dilute Bose gas in a random external potential .
Bose-Einstein condensation and superfluidity of dilute Bose gas in a random potential
In Vycor glass, the atoms are adsorbed and fully cover the surfaces of the open pores due to the van der waals attraction.
Bose-Einstein condensation and superfluidity of dilute Bose gas in a random potential
Because the ﬁrst layer of 4He adsorbed on the surfaces cannot move and behaves as a solid, we assume the pore size 30˚A of Vycor glass is effectively reduced by 2a.
Bose-Einstein condensation and superfluidity of dilute Bose gas in a random potential
It is presumed to describe equilibrium phase transitions in physical systems such as ﬂuids adsorbed in porous media and diluted antiferromagnets.
Ground state numerical study of the three-dimensional random field Ising model
We comment and discuss the ﬁndings and conclusions of a recent theoretical study of the diffraction of He atoms from a monolayer of Xe atoms adsorbed on the graphite (0001) surface [Khokonov et al., Surf.
Diffraction of He atoms from Xe monolayer adsorbed on the graphite (0001) revisited: The importance of multiple scattering processes
In a recent Letter1 and subsequent Erratum2 Khokonov, Kokov and Karamurzov1 (hereafter to be referred to as KKK) treated the problem of He atom scattering (HAS) from an ordered monolayer of Xe atoms adsorbed on the (0001) surface of graphite (Gr).
Diffraction of He atoms from Xe monolayer adsorbed on the graphite (0001) revisited: The importance of multiple scattering processes
While the long-range forces between substrate and adsorbate are responsible for the critical transition, which occurs at the temperature at which the Hamaker constant changes sign, it is primarily the short-range components of the forces that bring about the ﬁrst-order transition.
Transition temperatures and contact angles in the sequential-wetting scenario of n-alkanes on (salt) water
This behavior follows from the leading terms of the tails of the long-range forces between substrate and adsorbate .
Transition temperatures and contact angles in the sequential-wetting scenario of n-alkanes on (salt) water
As mentioned above, the true wetting transition to complete wetting is continuous and brought about by long-range forces between substrate and adsorbate, which change their nature from inhibiting complete wetting to supporting it at this temperature, Tw ,c .
Transition temperatures and contact angles in the sequential-wetting scenario of n-alkanes on (salt) water
***