Готові списки джерел за темами / Surface and interfaces

Добірка наукової літератури з теми "Surface and interfaces"

Автор: Grafiati
Опубліковано: 6 вересня 2023
Оновлено: 25 травня 2024

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Статті в журналах з теми "Surface and interfaces"

1

Chan, Chi-Ming, Lu-Tao Wang, and Lin Li. "Applications of Surface Analysis Techniques in Surface Characterization of Polymer Surfaces and Interfaces." Journal of The Adhesion Society of Japan 38, no. 5 (2002): 173–92. http://dx.doi.org/10.11618/adhesion.38.173.

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2

Chen, Xiaobin, Jiasheng Zhang, Yuanjie Xiao, and Jian Li. "Effect of roughness on shear behavior of red clay – concrete interface in large-scale direct shear tests." Canadian Geotechnical Journal 52, no. 8 (August 2015): 1122–35. http://dx.doi.org/10.1139/cgj-2014-0399.

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Few studies have focused on evaluating regular surface roughness and its effect on interfacial shear behavior of the red clay – concrete interface. This paper presents the results of a series of laboratory large-scale direct shear tests conducted using different types of red clay – concrete interfaces. The objective is to examine the effect of surface roughness on these types of soil–concrete interfaces. In the smooth-interface tests, the measured peak and residual shear strength values are very close to each other, with no observed shear dilation. The surface roughness is found to have a remarkable effect on the interfacial shear strength and shear behavior, with the shear strength increasing with increased surface roughness level. The shear dilation is likely to occur on rougher interfaces under lower confining pressure due to the behavior of compressed clay matrices. Owing to the clay matrix’s cohesion and friction, the interfacial shear strength on rough interfaces consists of cohesive and frictional forces between the clay and concrete surfaces. The friction angle value is observed to fluctuate between the clay’s friction angle and the smooth interface’s friction angle. This can be related to the position change of the shear failure slip plane. The confining pressure and surface roughness could change the shear failure plane’s position on the interface. Furthermore, the red clay – structure interface is usually known as the weakest part in the mechanical safety assessment.
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3

Marecek, Vladim^ ^iacute;r. "Surface Layers at the Polarized Liquid/Liquid Interfaces." Review of Polarography 60, no. 1 (2014): 17–24. http://dx.doi.org/10.5189/revpolarography.60.17.

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4

Robinson, I. K. "Surface Structural Techniques Applied to Interfaces." MRS Bulletin 15, no. 9 (September 1990): 38–41. http://dx.doi.org/10.1557/s0883769400062436.

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An interface is an internal surface, the boundary between two media which may be crystalline, amorphous solid, or liquid. Its close similarity with a surface, a solid-vacuum boundary, suggests that many of the powerful techniques available for studying surfaces might be applied to the interface structure problem. The extent to which this is possible is the subject of this article.The techniques to be discussed in this article include low energy electron diffraction (LEED), medium energy ion scattering (MEIS), x-ray diffraction, and x-ray reflectivity. (The most widely used method, transmission electron microscopy (TEM), is the subject of a separate article in this issue of the MRS BULLETIN.) To summarize what we will find, surface methods were developed to be nonpenetrating in order to have surface sensitivity. This works against us in the interface situation by requiring the use of extremely thin samples, at least on one side of the interface. This means special handling of samples in some cases and raises the possibility of artifac-tual results. Of the three methods, x-ray diffraction is the most penetrating and least surface sensitive; it probably has the greatest potential for widespread use in interface science.This article defines structure as “atomic structure” for this purpose: we are interested in the coordinates of atoms at the interface and their relation to bulk structures on one or both sides. For this reason, we will consider only interfaces that are crystalline on at least one side. Since crystals are by far our strongest structural reference point, much less can be said about other interfaces. We will also consider the morphology of an interface, defined as the boundary of the crystal(s) that demarcates the interface, also at the atomic level. This is most apparent in the form of interface roughness. The roles of strain and misfit dislocations in interface formation, also studied by these techniques, are outside the scope of this article.
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5

Li, Junbai, and Krister Holmberg. "Surface chemistry and interface science." Physical Chemistry Chemical Physics 19, no. 35 (2017): 23568–69. http://dx.doi.org/10.1039/c7cp90152f.

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6

Weidner, Elizabeth, and Thomas C. Weber. "Broadband acoustic characterization of backscattering from a rough stratification interface." Journal of the Acoustical Society of America 155, no. 1 (January 1, 2024): 114–27. http://dx.doi.org/10.1121/10.0024148.

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Broadband acoustic analysis of scattering from sharp density gradients in the water column generally treat the interfaces as smooth surfaces. However, these interfaces may exhibit roughness owing to external water column forcing and local convective processes. In this work we extend broadband backscatter analysis methods to consider interface roughness by drawing upon methods developed for sea surface and seabed acoustic backscattering. The one-dimensional acoustic model from Weidner and Weber [J. Acoust. Soc. Am. 150(6), 4353–4361 (2021)], which predicts a decay in the reflected wave amplitude from stratification interfaces with increasing frequency, was expanded for surface applications. The expanded model was used to analyze the scattered pressure field from interfaces over a range of surface roughness magnitudes. Analysis of model results indicate that stratification interface roughness, quantified by the root-mean-squared interface slope angle and root-mean-squared height of the interface, modifies the model-predicted frequency-dependent backscattering. A broadband acoustic inversion procedure to remotely measure the magnitude of the vertical extent of stratification gradients and the corresponding sound speed perturbation was defined. The broadband inversion method was tested on data collected in the Baltic Sea with well-documented, strong salinity-driven stratification.
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7

Robinson, I. K. "Surface diffraction on semiconductor surfaces and interfaces." Applied Surface Science 56-58 (January 1992): 117–22. http://dx.doi.org/10.1016/0169-4332(92)90224-l.

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You, Hoydoo, and Zoltán Nagy. "Applications of Synchrotron Surface X-Ray Scattering Studies of Electrochemical Interfaces." MRS Bulletin 24, no. 1 (January 1999): 36–40. http://dx.doi.org/10.1557/s088376940005171x.

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Aqueous-solution/solid interfaces are ubiquitous in modern manufacturing environments as well as in our living environment, and studies of such interfaces are an active area of science and engineering research. An important area is the study of liquid/solid interfaces under active electrochemical control, which has many immediate technological implications, for example, corrosion/passivation of metals and energy storage in batteries and ultracapacitors. The central phenomenon of electrochemistry is the charge transfer at the interface, and the region of interest is usually wider than a single atomic layer, ranging from a monolayer to thousands of angstroms, extending into both phases.Despite the technological and environmental importance of liquid/solid interfaces, the atomic level understanding of such interfaces had been very much hampered by the absence of nondestructive, in situ experimental techniques. The situation has changed somewhat in recent decades with the development of the largely ex situ ultrahigh vacuum (UHV) surface science, modern spectroscopic techniques, and modern surface microscopy.However in situ experiments of electrochemical interfaces are difficult, stemming from the special nature of these interfaces. These are so-called buried interfaces in which the solid electrode surface is covered by a relatively thick liquid layer. For this reason, the probe we use in the structural investigation must satisfy simultaneously two conditions: (1) the technique must be surface/interface sensitive, and (2) absorption of the probe in the liquid phase must be sufficiently small for penetration to and from the interface of interest without significant intensity loss.
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9

Li, Huanhuan, Zhigang Meng, and Songlin Shen. "Effects of Interface Morphology on the Shear Mechanical Properties of Sand–Concrete Interfaces." Materials 16, no. 18 (September 8, 2023): 6122. http://dx.doi.org/10.3390/ma16186122.

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The morphology of the contact surface between cast-in-place engineering structures and soil is generally random. Previous research focusing on the shear mechanical properties of soil–concrete interfaces has predominantly concentrated on the role of interface roughness by constructing regular concrete surface types, largely neglecting the potential impact of the roughness morphology (i.e., the morphology of the concrete surface). In this study, concrete blocks with the same interface roughness and different roughness morphologies were constructed based on the sand-cone method, including random rough surface, triangular groove surface, rectangular groove surface, trapezoid groove surface, and semicircular groove surface. A series of direct shear tests were conducted on the rough and smooth sand–concrete interfaces, as well as on natural sand. Through these tests, we examined the shear mechanical behavior and strength of the sand–concrete interfaces, and analyzed the underlying shear mechanisms. The results showed that: (i) the interface morphology had little effect on the variation in the shear stress–displacement curve of sand–concrete interfaces, and it had a significant influence on the shear strength of the interfaces; (ii) under the same normal stress, the shear strength of the sand–concrete interfaces with a random rough surface was the greatest, followed by the triangular groove surface, while the shear strength of the rectangular groove surface proved the lowest; (iii) the shear strength of the sand–concrete interfaces with the same roughness was affected by the size of the contact area between the concrete plane and the sand, that is, a larger contact area correlated with a decrease in shear strength. It can be concluded that the shear strength value of a sand–concrete surface with the triangular groove is the closest to the shear strength of a random rough interface. By gaining a deep understanding of the effects of different contact surface morphologies on shear strength and shear behavior, significant insights can be provided for optimizing engineering design and enhancing engineering performance.
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10

Zhang, Hengzhong, and Jillian F. Banfield. "Phase transformation of nanocrystalline anatase-to-rutile via combined interface and surface nucleation." Journal of Materials Research 15, no. 2 (February 2000): 437–48. http://dx.doi.org/10.1557/jmr.2000.0067.

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The kinetics of phase transformation of nanocrystalline anatase samples was studied using x-ray diffraction at temperatures ranging from 600 to 1150 °C. Kinetic data were analyzed with an interface nucleation model and a newly proposed kinetic model for combined interface and surface nucleation. Results revealed that the activation energy of nucleation is size dependent. In anatase samples with denser particle packing, rutile nucleates primarily at interfaces between contacting anatase particles. In anatase samples with less dense particle packing, rutile nucleates at both interfaces and free surfaces of anatase particles. The predominant nucleation mode may change from interface nucleation at low temperatures to surface nucleation at intermediate temperatures and to bulk nucleation at very high temperatures. Alumina particles dispersed among the anatase particles can effectively reduce the probability of interface nucleation at all temperatures.
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Дисертації з теми "Surface and interfaces"

1

Dahal, Arjun. "Surface Science Studies of Graphene Interfaces." Scholar Commons, 2015. http://scholarcommons.usf.edu/etd/5820.

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Interfaces between graphene and dissimilar materials are needed for making devices, but those interfaces also modify the graphene properties due to charge transfer and/or symmetry breaking. In this dissertation we investigate the technology of preparing graphene on different substrates and how the substrate influences the electronic properties of graphene. Synthesizing large area graphene on late transition metals by chemical vapor deposition is a promising approach for many applications of graphene. Among the transition metals, nickel has advantages because the good lattice match and strong interaction between graphene/Ni(111) enables the synthesis of a single domain of graphene on Ni(111). However, the nickel substrate alters the electronic structure of graphene due to substrate induced symmetry breaking and chemical interaction of the metal d-band with graphene. Similar chemical interactions are observed for other transition metals with a d-band close to the Fermi-level. On the other hand, graphene mainly physisorbs on transition metals with a lower lying d-band center. In this thesis we investigate the growth of graphene on nickel by vacuum chemical vapor deposition (CVD). In particular, we present our studies of graphene synthesis on Ni(111) substrates. We demonstrate the self-limiting monolayer of single domain of graphene can be grown on single crystal Ni(111). Our studies also show that selective twisted bilayer graphene can be grown by carbon segregation on Ni(111)-films. To modify the interaction between graphene and the nickel substrate we investigated the intercalation of tin. In the case of graphene physisorbed on weakly interacting metals, some charge doping of graphene occurs due to work function differences between graphene and the metal. Using x-ray photoemission spectroscopy (XPS) we correlate the charge doping of graphene on different metals with the C-1s binding energy. This study demonstrate that XPS can be used to determine the Fermi-level in graphene. While metal intercalation can alter the interaction with the substrate it does not avoid overlap of electronics states at the Fermi-level. Therefore a band gap material should be inserted between the graphene and the metal growth substrate (in this case Pt(111)). This is accomplished by oxidation of intercalated iron at elevated oxygen pressure. We demonstrate that a 2D-FeO layer can be formed in between graphene and the Pt(111) surface. We discuss the role of the 2D-FeO moiré-structure on the nanoscale electronic properties of graphene. To date good quality graphene can only be grown by CVD on late transition metals. To obtain graphene on other substrates the graphene can be transferred mechanically from a growth substrate to various other materials. We demonstrate that this transfer can also be achieved to tungsten, an early transition metal that easily forms a carbide. In our studies to avoid oxidation of the tungsten substrate and reaction of the graphene with the tungsten substrate under thermal treatment, protection of the W(110) surface with sulfur has been explored. For the integration of graphene into device architectures, graphene has to be interfaced with high-κ dielectrics. However, because of the inert nature of graphene, most high-κ do not wet graphene and thus preventing formation of contiguous dielectric layers. Yttrium oxide (Y2O3) has been demonstrated to be an exception and we characterized the growth of Y2O3 on various metal supported graphene and graphene transferred to SiO2. We showed that such a Y2O3 layer can also act as seeding layer for the growth of alumina, which is the preferred dielectric material in many applications. Finally, we investigate the charge doping of graphene in a metal/graphene/dielectric stack and find that the charge doping of graphene is a function of both the work function of the metal as well as the covering dielectric. Thus the dielectric layer can modify the charge doping of graphene at a metal contact.
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2

Purcell, Isabella Pauline. "Specular reflection from interfaces." Thesis, University of Oxford, 1994. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.386624.

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3

Hazell, Gavin D. A. "Surface scattering from soft matter at interfaces." Thesis, University of Bath, 2014. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.642031.

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The aim of this work has been to make use of surface scattering techniques to study soft matter at interfaces. The work presented herein is composed of two distinct bodies of work. The first comprises a fundamental study of the physical and structural properties of Langmuir monolayers composed of sulfobetaine surfactants. Physiochemical properties of the films have been investigated through the use of Langmuir trough techniques. This has been used to support x-ray and neutron reflectometry data, from which structural parameters were derived. The second body of work involves attempts to find and/or characterize novel ways of aligning proteins at interfaces. Soluble proteins at lipid interfaces have been characterized in terms of their interactions with functionalized lipid monolayers. Specific interactions have been utilized to adsorb protein layers at the interface through interactions with His-tag chelating lipids within the monolayer. These have been characterized using neutron reflectometry and quartz crystal microbalance studies. Work has also been completed to design a suitable system for the adsorption of membrane proteins. This has involved aligning phospholipid bilayer nanodiscs at the lipid interface and subsequent characterization through neutron reflectometry.
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4

Wu, Liuming. "Surface complexation at calcium mineral-water interfaces." Doctoral thesis, Luleå, 1994. http://urn.kb.se/resolve?urn=urn:nbn:se:ltu:diva-25727.

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Surface reactions occurring at solid-water interfaces in calcium mineral-ligands systems have been studied. Both hydrous apatite and fluorite surfaces show clear amphoteric properties. An ion exchange process between lattice ions of F- on fluorite and OH- ions in bulk solution is discovered. The surface adsorption of Alizarin Red S and sodium oleate are determined. Surface chemical reaction models are established based on acidbase potentiometric titrations, solubility, adsorption and zeta-potential measurements in 0. 1 mol dm-3 ionic media at 25'C. Experimental data are evaluated using the computer program FITEQL assuming a constance capacitance model for the electric double layer. Surface complexes identities are obtained from FT-IR, FT-Raman, and UV/visible spectroscopy studies. A series of surface equilibrium constants in the system are presented. The correlation between surface complex formation and mineral flotation is discussed.
Godkänd; 1994; 20070429 (ysko)
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5

Maeda, Nobuo, and nobuo@engineering ucsb edu. "Phase Transitions of Long-Chain N-Alkanes at Interfaces." The Australian National University. Research School of Physical Sciences and Engineering, 2001. http://thesis.anu.edu.au./public/adt-ANU20011203.151921.

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An experimental study of phase transitions of long-chain n-alkanes induced by the effect of interfaces is described. ¶ The phase behaviour of long-chain n-alkanes (carbon number 14, 16, 17, 18) adsorbed at isolated mica surfaces and confined between two mica surfaces has been studied in the vicinity of and down to several degrees below the bulk melting points, Tm. Using the Surface Force Apparatus we have measured the thickness of alkane films adsorbed from vapour (0.97 [equal to or greater-than] p/p[subscript o] [equal to or greater-than] 0.997), studied capillary condensation transition, subsequent growth of capillary condensates between two surfaces, and phase transitions in both the adsorbed films and the condensates. By measuring the growth rate of the capillary condensates we have identified a transition in the lateral mobility of molecules in the adsorbed films on isolated mica surfaces. This transition to greater mobility occurs slightly above Tm for n-hexadecane, n-heptadecane and n-octadecane but several degrees below Tm for n-tetradecane, and is accompanied by a change in wetting behaviour and a measurable decrease in adsorbed film thickness for n-heptadecane and n-octadecane. Capillary condensates that form below Tm remain liquid, but may freeze if the degree of confinement is reduced by separation of the mica surfaces. An increase in the area of the liquid-vapour interface relative to that of the liquid-mica interface facilitates freezing in the case of the long-chain alkanes, which show surface freezing at the liquid-vapour interface. ¶ Although thermodynamic properties of the surface freezing transition have been rather well documented, the kinetics involved in formation of such ordered monolayers has so far received very little attention. We studied the surface tension of n-octadecane as a function of temperature in the vicinity of Tm, using the static Wilhelmy plate and the dynamic maximum bubble pressure methods. The two methods give different results on cooling paths, where nucleation of the surface ordered phase is involved, but agree on heating paths, where both methods measure properties of the equilibrium surface phase. On cooling paths, the surface of bubbles may supercool below the equilibrium surface freezing temperature. The onset of surface freezing is marked by a sharp drop in the surface tension. The transition is accompanied by an increased stability of the films resulting in longer bubble lifetimes at the liquid surface, which suggests that the mechanical properties of the surfaces change from liquid-like to solid-like. Our results suggest occurrence of supercooling of the monolayer itself.
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6

Li, Zhi Xin. "Neutron reflection from interfaces." Thesis, University of Oxford, 1996. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.320621.

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7

Johnson, Edward G. "Dynamics of interfaces and detergency." Thesis, Queen's University Belfast, 1997. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.361250.

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8

Bennett, Andrew Michael. "Properties, processes and surface chemistry at diamond interfaces." Thesis, University of Oxford, 2005. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.434867.

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9

Al-Bermany, Ehssan. "Polymer/graphene oxide nanocomposites : surface adsorption and interfaces." Thesis, University of Sheffield, 2017. http://etheses.whiterose.ac.uk/18510/.

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10

Iscimen, Mehmet. "Shearing Behavior Of Curved Interfaces." Thesis, Georgia Institute of Technology, 2004. http://hdl.handle.net/1853/7256.

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The frictional behavior of soil-construction material interfaces is of significant importance in geotechnical engineering applications such as retaining structures, pile foundations, geosynthetic liners, and trenchless technologies. Since most failures initiate and develop on the interfaces, special attention is required to predict the capacity of these weak planes in the particular application. Pipe-jacking and microtunneling technologies are being more widely used over the past decade and there is significant interest to predict the jacking forces and jacking distances achievable in order to achieve more efficient design and construction. This study focuses on the evaluation of the frictional characteristics and factors affecting the shear strength of pipe-soil interfaces. Eight different pipes made from fiber reinforced polymer (FRP), polycrete, steel, concrete, and vitrified clay were tested in the experimental program. For this purpose, a new apparatus was designed to conduct conventional interface direct shear testing on pipes of different curvature. This device allows coupons cut from actual conduits and pipes to be tested in the laboratory under controlled conditions. The apparatus includes a double-wall shear box, the inner wall of which is interchangeable to allow for testing against surfaces of different curvatures. By considering a narrow width section, the circular interface of pipes was approximated with a surface along the axial direction and the boundary is defined by the inner box. Roughness tests were performed using a stylus profilometer to quantify the surface characteristics of the individual pipes and relate these to the interface shear behavior. The surface topography showed different degrees of variability for the different pipes. To extend the range of roughness values tested and force the failure to occur in the particulate media adjacent to the interface, two artificial pipe surfaces were created using rough sandpapers. Interface shear tests were performed using the new apparatus with air-pluviated dense specimens of Ottawa 20/30 sand. Additional tests were performed using Atlanta blasting sand to evaluate the effect of particle angularity. The effect of normal stress and relative density were also examined. The interface strength was shown to increase with surface roughness and finally reach a constant value above a certain critical roughness value, which corresponded to the internal strength of the soil itself. This represented the failure location moving from the interface into the soil adjacent to the interface. Both the strength and the shearing mechanism were thus affected by the surface topography. It was also shown that the interface shear strength was affected by particle angularity, relative density and normal stress.
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Книги з теми "Surface and interfaces"

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Ecole, d'été de physique théorique (Les Houches Haute-Savoie France) (48th 1988). Liquides aux interfaces =: Liquids at interfaces. Amsterdam: North-Holland, 1990.

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2

P, Grange, Delmon Bernard, Université catholique de Louvain (1970- ). Institut interfacultaire des sciences naturelles appliquées., and Université catholique de Louvain (1970- ).Centre de recherche des matériaux avancés., eds. Interfaces in new materials. London: Elsevier Applied Science, 1991.

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3

Mönch, Winfried. Semiconductor surfaces and interfaces. 2nd ed. New York: Springer-Verlag, 1995.

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4

Semiconductor surfaces and interfaces. 3rd ed. Berlin: Springer, 2001.

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5

Mönch, Winfried. Semiconductor surfaces and interfaces. 2nd ed. Berlin: Springer-Verlag, 1995.

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6

Mönch, Winfried. Semiconductor surfaces and interfaces. Berlin: Springer-Verlag, 1993.

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7

Jacek, Lipkowski, and Ross P. N, eds. Structure of electrified interfaces. New York, N.Y: VCH Publishers, 1993.

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8

A, Hiraki, ed. Metal-semiconductor interfaces. Tokyo, Japan: Ohmsha, 1995.

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9

Laude, L. D. Interfaces Under Laser Irradiation. Dordrecht: Springer Netherlands, 1987.

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10

author, Graf Kh (Karlheinz), and Kappl Michael 1963 author, eds. Physics and chemistry of interfaces. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA, 2013.

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Частини книг з теми "Surface and interfaces"

1

Derjaguin, B. V., N. V. Churaev, and V. M. Muller. "Forces Near Interfaces." In Surface Forces, 1–23. Boston, MA: Springer US, 1987. http://dx.doi.org/10.1007/978-1-4757-6639-4_1.

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2

Fauve, S. "Waves on Interfaces." In Free Surface Flows, 1–44. Vienna: Springer Vienna, 1998. http://dx.doi.org/10.1007/978-3-7091-2598-4_1.

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3

Miyamae, Takayuki, and Kouki Akaike. "Analysis of Molecular Surface/Interfacial Layer by Sum-Frequency Generation (SFG) Spectroscopy." In Interfacial Phenomena in Adhesion and Adhesive Bonding, 291–360. Singapore: Springer Nature Singapore, 2023. http://dx.doi.org/10.1007/978-981-99-4456-9_5.

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AbstractThis chapter reviews recent progress in polymer surfaces and interface studies using sum-frequency generation (SFG) vibrational spectroscopy. SFG is a surface-specific vibrational spectroscopic technique that has spread on a worldwide scale since it was first reported in 1987. The SFG principles, instruments, techniques, and experiments are presented in detail, and recent results on interfacial physics and chemistry at jointed interfaces are described. It focuses on SFG studies of the surfaces and buried interfaces of polymeric materials, such as modification of polymer surfaces, polymer-water, polymer-metal, and polymer–polymer interfaces. This review demonstrates that SFG is a powerful technique for nondestructive, in situ measurement of molecular level understanding at complex polymer surfaces and interfaces.
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Mönch, Winfried. "Surface States." In Semiconductor Surfaces and Interfaces, 33–57. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/978-3-662-04459-9_3.

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Mönch, Winfried. "Surface States." In Semiconductor Surfaces and Interfaces, 30–50. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-662-02882-7_3.

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6

Mönch, Winfried. "Surface States." In Semiconductor Surfaces and Interfaces, 31–53. Berlin, Heidelberg: Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-662-03134-6_3.

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7

Stenzel, Olaf. "Planar Interfaces." In Springer Series in Surface Sciences, 97–129. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-21602-7_6.

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8

Lüth, Hans. "Surface Phonons." In Surfaces and Interfaces of Solids, 218–53. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-662-10159-9_5.

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9

Blakely, J. M., and C. C. Umbach. "Surface Self-Diffusion, Capillarity, and Surface Steps." In Diffusion at Interfaces: Microscopic Concepts, 102–10. Berlin, Heidelberg: Springer Berlin Heidelberg, 1988. http://dx.doi.org/10.1007/978-3-642-73632-2_11.

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10

George, Michael, Wolfgang J. Parak, and Hermann E. Gaub. "Highly Integrated Surface Potential Sensors." In Bio-Nano Interfaces, 17–40. New York: Jenny Stanford Publishing, 2024. http://dx.doi.org/10.1201/9781003306498-2.

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Тези доповідей конференцій з теми "Surface and interfaces"

1

Wang, Ding-Sheng, and Dian-Hong Shen. "Lectures on Solid Surfaces and Interfaces." In International School on Surface Physics. WORLD SCIENTIFIC, 1990. http://dx.doi.org/10.1142/9789814540155.

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2

Hemmert, Fabian. "Interfaces beyond the surface." In the 28th of the international conference extended abstracts. New York, New York, USA: ACM Press, 2010. http://dx.doi.org/10.1145/1753846.1753881.

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3

Gaul, L., and M. Mayer. "Efficient modelling of contact interfaces of joints in built-up structures." In CONTACT/SURFACE 2007. Southampton, UK: WIT Press, 2007. http://dx.doi.org/10.2495/secm070191.

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4

Dreyssé, H., A. Vega, D. Stoeffler, J. Khalifeh, and C. Demangeat. "Magnetism of transition metal overlayers: Fe/Cr stepped interfaces." In The 8th Latin American congress on surface science: Surfaces , vacuum, and their applications. AIP, 1996. http://dx.doi.org/10.1063/1.51139.

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5

Ronnow, D., M. Bergkvist, A. Roos, and C.-G. Ribbing. "Determination of Interface Roughness Using A Wavelength Scanning TIS Instrument." In Surface Roughness and Scattering. Washington, D.C.: Optica Publishing Group, 1992. http://dx.doi.org/10.1364/surs.1992.stub7.

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Анотація:
Optical scattering from surface micro irregularities at a specific wavelength is directly related to the RMS-roughness value of the surface1. It is usually measured by a TIS (Total Integrated Scatter) instrument. In its’ conventional application this method can only be used to investigate the front surface of opaque samples. In the case of transparent samples or samples coated with a transparent film, one must handle two scattering interfaces as well as possible interference effects in the film. The resulting light scattering cannot be described by the standard TIS equation. By combining the scalar scattering theory with the Fresnel formalism we have obtained a model which predicts the scattering from a double layer as a function of wavelength. By fitting model calculations to experimental scattering spectra with the interface roughness values as parameters we can extract the rms-roughness values of the two interfaces. The model has been described elsewhere2. Using the scattering spectra and such fitting calculations we can conveniently, and non-destructively, determine the RMS-roughness of a "hidden" interface.
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6

Takayama, O., E. Shkondin, M. E. Aryaee Panah, T. Repan, R. Malureanu, F. Jensen, and A. V. Lavrinenko. "Surface waves on metamaterials interfaces." In 2016 10th International Congress on Advanced Electromagnetic Materials in Microwaves and Optics (METAMATERIALS). IEEE, 2016. http://dx.doi.org/10.1109/metamaterials.2016.7746486.

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7

Mansouri, M., and M. M. Khonsari. "Surface Temperature in Oscillating Sliding Interfaces." In ASME/STLE 2004 International Joint Tribology Conference. ASMEDC, 2004. http://dx.doi.org/10.1115/trib2004-64391.

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Анотація:
A model is developed to predict the behavior of two sliding bodies undergoing oscillatory motion. A set of four dimensionless groups is introduced to characterize the transient dimensionless surface temperature rise. They are: the Peclet number Pe, the Biot number Bi, the amplitude of oscillation A, and the Hertzian semi-contact width α. Also considered in the analysis is the effect of the ratio β = A/α of the amplitude to the semi-contact width. The results of a series of simulations, covering a range of these independent parameters, are presented and examples are provided to illuminated the utility of the model.
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8

Avrahami, Daniel, Mitesh Patel, Yusuke Yamaura, and Sven Kratz. "Below the Surface." In IUI'18: 23rd International Conference on Intelligent User Interfaces. New York, NY, USA: ACM, 2018. http://dx.doi.org/10.1145/3172944.3172962.

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9

Pancholi, Lokesh. "Squeak Behavior of Plastic Interfaces." In International Conference on Advances in Design, Materials, Manufacturing and Surface Engineering for Mobility. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2019. http://dx.doi.org/10.4271/2019-28-0083.

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10

Baniecki, J. D., M. Ishii, K. Kurihara, and K. Yamanaka. "Surface and Interface Chemistry of Epitaxial BST Films and Pt/BST Interfaces." In 2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics. IEEE, 2007. http://dx.doi.org/10.1109/isaf.2007.4393206.

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Звіти організацій з теми "Surface and interfaces"

1

Jennings, G. Kane. Surface-Directed Fabrication of Integrated Membrane-Electrode Interfaces. Office of Scientific and Technical Information (OSTI), December 2013. http://dx.doi.org/10.2172/1108612.

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2

Dai, Weitao. Surface modes at metallic an photonic crystal interfaces. Office of Scientific and Technical Information (OSTI), January 2009. http://dx.doi.org/10.2172/985309.

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3

Tsukruk, Vladimir V. Design of Bio-Hybrid Surface Assemblies at Engineering Interfaces. Fort Belvoir, VA: Defense Technical Information Center, May 2005. http://dx.doi.org/10.21236/ada435743.

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4

Schultz, Sheldon. A New Approach to Understanding the Semiconductor Surface and Interfaces. Fort Belvoir, VA: Defense Technical Information Center, October 1988. http://dx.doi.org/10.21236/ada200131.

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5

Miller, R. J. D. Ultrafast optical studies of surface reaction processes at semiconductor interfaces. Office of Scientific and Technical Information (OSTI), November 1991. http://dx.doi.org/10.2172/6066821.

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6

Richmond, Geraldine L., and Stephen D. Kevan. Nonlinear Studies of Surface and Interfaces of Advanced Semiconductor Materials. Fort Belvoir, VA: Defense Technical Information Center, July 1992. http://dx.doi.org/10.21236/ada253365.

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7

Miller, R. J. D. Ultrafast optical studies of surface reaction processes at semiconductor interfaces. Office of Scientific and Technical Information (OSTI), March 1993. http://dx.doi.org/10.2172/6668112.

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8

Blakely, J. Surface phases and their influence on metal-oxide interfaces. Progress report. Office of Scientific and Technical Information (OSTI), January 1993. http://dx.doi.org/10.2172/10176330.

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9

Miller, R. J. D. Ultrafast optical studies of surface reaction processes at semiconductor interfaces. Progress report. Office of Scientific and Technical Information (OSTI), October 1994. http://dx.doi.org/10.2172/10191250.

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10

Blackely, J. H. Surface phases and their influence on metal-oxide interfaces: Progress report, 1 April 1989. Office of Scientific and Technical Information (OSTI), March 1989. http://dx.doi.org/10.2172/6117196.

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