• Proceedings of the Korean Vacuum Society Conference
• /
• 1999.07a
• /
• pp.170-170
• /
• 1999

We studied Nb growth mode on Cu(100) surface by scanning tunneling microscopy (STM) at room temperature. Nb/Cu is immiscible at room temperature and thus is an ideal system for studying surface alloy formation. Initially deposited Nb atoms are incorporated subsurface on Cu(100). After annealing, they are preferentially found at step edges and appear as bright dots surrounded by dark rings. Ordering emerges from step edges as annealed. Ordered ({{{{ SQRT { 5} }$\times${{{{ SQRT { 5} }}}})R 26.6$^{\circ}$phase Nb structure is formed at $\theta$<0.2ML after annealing to 50$0^{\circ}C$. At higher coverage, $\theta$>0.25, annealing leads to p(2$\times$2) phase. due to large mismatch in lattice parameters, the domain is limited to a few tens of nm2. Growth kinetics of the system will be discussed.

• Journal of the Korean Vacuum Society
• /
• v.1 no.1
• /
• pp.1-10
• /
• 1992

Three chemical precleaning methods-degreasing, electropolishing and acidic etching-suitable for stainless steel vacuum chamber have been studied and compared. The techniques used in evaluating and comparing the three treatments include Auger analysis and the measurement of the outgassing rate. The obtained outgassing rates (N2 equivalent) are 1.1 $\times$ 10-10torr l/s cm2 and 3.9 $\times$ 10-11torr l/s cm2 for degreasing electropolishing, and etching method, respectively, after 48 hours from the initial pumpdown at room temperature. A simple model is introduced to analyze the pumpdown curve. Some surface parameters, such as surface coverage, mean residence time, and desorption energy, are calculated from corresponding equations derived from this model.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2012.02a
• /
• pp.280-280
• /
• 2012

We examined ammonia diffusion on the surface of amorphous ice film through the measurement of decreasing residual quantity of $NH_3$ molecules compared to $H_2O$. The populations of $NH_3$ molecules on the surface of amorphous ice were monitored by using the techniques of temperature programmed reactive ion scattering (TPRIS) method. The ratio of intensity between ammonia and water was examined as a function of time at controlled temperature. When ammonia molecules were externally added onto an ice film at a temperature of 80 K, ammonia coverage with regard to ice was 0.12-0.16 ML. The intensity of ammonia molecules on the surface of ice decreased as time increased and the extent of decreased intensity of ammonia increased as controlled temperature increased. Moreover, energy barrier was estimated to be $51kJmol^{-1}$ on amorphous ice film. The results of the experiment indicate that ammonia molecules have a property of vertical diffusion into amorphous ice and the energy barrier of ammonia diffusion into bulk of ice is higher than that of hydrogen bonding.

• Proceedings of the Korea Association of Crystal Growth Conference
• /
• 1996.06b
• /
• pp.129-153
• /
• 1996

In aqueous slurry processing of silicon nitride, the interaction of dispersant and binder on the surface of particles was studied to identify the effect of these additives on ceramic powder processing. Polymethacrylic acid (PMAA) and polyvinyl alcohol (PVA) were used as dispersant and binder, respectively. the adsorption isotherms of PMAA and PVA for the silicon nitride suspension were determined, while the adsorption of PMAA was differentiated in the mixed additive system by ultraviolet spectroscopy. These experiments were done in order to investigate the effect of these organic additives on the physicochemical properties of silicon nitride suspensions. The electrokinetic behavior of silicon nitride was subsequently measured by electrokinetic sonic amplitude (ESA). As PMAA adsorbed onto silicon nitride, the isoelectric point (pHicp) shifted from pH=6.7 to acidic pH, depending on the surface coverage of PMAA. However, adsorption of PVA did not change the pHicp of suspensions, but did decrease the surface potential of silicon nitride moderately. The rheological behavior of silicon nitride suspensions was measured to assess the stability of particles in aqueous media, and was correlated with the electrokinetic behavior and adsorption isotherm data for silicon nitride.

• Journal of the Korean institute of surface engineering
• /
• v.29 no.5
• /
• pp.350-356
• /
• 1996

This paper presents VHF-Plasma Enhanced Chemical Vapor Deposition (VHF-PECVD) of Ti/TiN with silne reduction process, using $TiCl_4$ source. VHF plasma, which is denser than a conventional RF plasma, produces a large number of radicals. Silane reduction process, which supplies silane radicals, more promotes dissociation of Ti-Cl bond than a conventional hydrogen reduction process. therefore, the VHF-PECVD with silane reduction process forms high quality Ti/TiN films, which have low level of Cl content(<0.2 at.%). In result, the resistivity for Ti or TiN is less than 200$\mu$$\Omega$cm. The surface morphology of Ti film is very smooth. The structure of TiN film is amorphous. Furthermore, excellent step coverage for the films is obtained.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2013.08a
• /
• pp.137-137
• /
• 2013

The most stable adsorption structures and their corresponding energies of 4-pyridone, 4-hydroxypyridine, 2-pyridone and 2-hydroxypyridine have been investigated by Density Functional Theory (DFT) calculation method and high-resolution photoemission spectroscopy (HRPES). We confirmed that between the two reaction centers of 4- and 2-pyridone, only O atom of carbonyl functional group can act as a Lewis base and thus, O dative bonding structure is the most stable. On the other hand, we clarified that both the two reaction centers (the cyclic N atom and the O atom of hydroxyl functional group) of 4- and 2-hydroxypyridine (tautomers of 4- and 2-pyridone) can successfully function as a Lewis base. Through the interpretation of the N 1s and O 1s core level spectra obtained using HRPES, we could confirm the electronic structures and bonding configurations of these molecules with a coverage dependence on the Ge(100) surface.

• Bulletin of the Korean Chemical Society
• /
• v.8 no.1
• /
• pp.19-26
• /
• 1987

A statistical thermodynamical treatment for polymer adsorption from solution is presented. The canonical partition function for the polymer solution in the presence of a surface or an impermeable interface is formulated on the basis of usual quasi-crystalline lattice model, Bragg-Williams approximation of random mixing, and Pak's simple treatment of liquid. The present theory gives the surface excess ${\Gamma}_{exc}$ and the surface coverage ${\phi}^s_2$ of the polymer as a function of the chain length x, the Flory-Huggins parameter x, the adsorption energy parameter $x_s$, and polymer concentration $v_2$. Present theory is also applicable to the calculation of interfacial tension of polymer solution against water. For the idealized flexible polymer, interfacial tensions according to our theory fit good to the experimental data to the agreeable degrees.

• Bulletin of the Korean Chemical Society
• /
• v.12 no.2
• /
• pp.138-143
• /
• 1991

Laser Raman spectroscopy has been used to study the interaction of $MoO_3$ with $TiO_2$. The bulk molybdenum oxide appeared to spread on the surface of titania under the submonolayer coverage. The surface polymolybdate was observed to be very stable with respect to the repeated treatment of reduction and subsequent calcination. Owing to the interaction of molybdate and titania, the phase transformation of $TiO_2$ seemed to be strongly retarded. The additives such as Co and Ni reacted readily with $MoO_3$ to form the corresponding molybdate salts. Nevertheless, the polymolybdate species appeared to be more stable on the titania surface than the molybdate salts.

• Asian Journal of Turfgrass Science
• /
• v.15 no.2
• /
• pp.39-50
• /
• 2001

This research was designed to develop the rapid propagation technology of zoysiagrass using carpet production and to provide turf-growing farmers with efficient cultivation methods thor carpet production. Turfgrass cultivar tested in cadet production by seeding was Z. japonica cv. Zenith. Since the surface coverage rate reached to 85% in 2 months after seeding at the rate 6g/$m^2$ in the early part of July, carpet production using ‘Zenith’seeds would be possible to produce within within the same year. Thrfgrasses tested in carpet production by vegetative propagation were Z. japonica, medium type Z. matrella, fine type Z. matrella, and medium type Z. japonica. Planting rates of vegetative parts (sprigs) were 1.2L/$m^2$, 2.4L/$m^2$, 2.5L/$m^2$, and 5L/$m^2$. Two different sizes of sprig were used; 1~2 nodes and 3~4 nodes. Surface coverage rate was 90% in one year after planting at the rate of 2.5L sprigs of medium type Z. japonica. Therefore, the use of sprigs with 3~4 nodes at the planting rate of 2.5L would be suitable for the carpet prodcution. Three months old zoysiagrass carpet (Zenith) was overseeded with Kentucky bluegrass, perennial ryegrass, and tall fescue at two different overseeding rate. Surface coverage rate was the highest (80%) at the plot overseeded with perennial ryegrass that showed the earliest germination. Suitable overseeding species for the rapid sod formation at the early stage of establishment were tall fescue and perennial ryegrass and desirable overseeding time was from early to middle of September.

• Journal of the Korean Electrochemical Society
• /
• v.2 no.2
• /
• pp.70-74
• /
• 1999

The electrode kinetic parameters at the Pd/0.5 M LiOH electrolyte interface have been qualitatively studied using the phase-shift method. The phase shift $(\phi)$ depends on both the cathode potential (E>0) and frequency (f), and $\theta$ is inversely proportional to the fractional surface coverage $\theta$. At an intermediate frequency (10 Hz), the phase-shift profile $(\phi\;vs.\;E)$ can be related to the fractional surface coverage $(\theta\;vs.\;E)$. The phase-shift method can be used to estimate or plot the Frumkin adsorption isotherm. The rate (r) of change of the free energy of adsorption with $({\theta})$ is 22.3 kJ/mol. The equilibrium constant (K) for adsorption and the standard free energy $({\Delta}G_{\theta})$ of the adsorbed hydrogen atom $(H_{ads})$ are $3.7\times10^{-3}{\Delta}G_{\theta}>-8.4kJ/mol$, respectively. For 1$0.38>\theta>0$, the energy liberation or the exothermic reaction for hydrogen adsorption at the Pd cathode can be occurred. The electrode kinetic parameters $(r,\;K,\;{\Delta}G_{\theta}$ depend on the fractional surface coverage $({\theta})$ or the phase shift $(\phi)$.