Journal articles on the topic 'Surface properties of condensed matter'

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1

Ritchie, R. H., and A. Howie. "Inelastic scattering at surfaces and interfaces." Proceedings, annual meeting, Electron Microscopy Society of America 44 (August 1986): 392–93. http://dx.doi.org/10.1017/s0424820100143560.

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An important part of condensed matter physics in recent years has involved detailed study of inelastic interactions between swift electrons and condensed matter surfaces. Here we will review some aspects of such interactions.Surface excitations have long been recognized as dominant in determining the exchange-correlation energy of charged particles outside the surface. Properties of surface and bulk polaritons, plasmons and optical phonons in plane-bounded and spherical systems will be discussed from the viewpoint of semiclassical and quantal dielectric theory. Plasmons at interfaces between dissimilar dielectrics and in superlattice configurations will also be considered.
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2

BOHR, HENRIK, JOHN H. IPSEN, and STEEN MARKVORSEN. "CONDENSED MATTER PHYSICS OF BIOMOLECULE SYSTEMS IN A DIFFERENTIAL GEOMETRIC FRAMEWORK." International Journal of Modern Physics B 21, no. 13n14 (May 30, 2007): 2475–92. http://dx.doi.org/10.1142/s0217979207043828.

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In this contribution biomolecular systems are analyzed in a framework of differential geometry in order to derive important condensed matter physics information. In the first section lipid bi-layer membranes are examined with respect to statistical properties and topology, e.g. a relation between vesicle formation and the proliferation of genus number. In the second section differential geometric methods are used for analyzing the surface structure of proteins and thereby understanding catalytic properties of larger proteins.
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3

Punkkinen, M. P. J., Q. M. Hu, S. K. Kwon, B. Johansson, J. Kollár, and L. Vitos. "Surface properties of 3dtransition metals." Philosophical Magazine 91, no. 27 (September 21, 2011): 3627–40. http://dx.doi.org/10.1080/14786435.2011.586953.

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4

Sehmbey, M. S., M. R. Pais, and L. C. Chow. "Effect of surface material properties and surface characteristics inevaporative spray cooling." Journal of Thermophysics and Heat Transfer 6, no. 3 (July 1992): 505–12. http://dx.doi.org/10.2514/3.389.

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5

Hamed, Rania, Daniel M. Schenck, and Jennifer Fiegel. "Surface rheological properties alter aerosol formation from mucus mimetic surfaces." Soft Matter 16, no. 33 (2020): 7823–34. http://dx.doi.org/10.1039/d0sm01232g.

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The effects of surface tension and surface viscoelastic properties on the formation of aerosol droplets generated from mucus-like viscoelastic gels (mucus mimetics) during shearing with a high velocity air stream were investigated.
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6

Tsvetkov, V. A., O. V. Tsvetkov, and V. A. Balandin. "Anisotropic Properties of the LC Surface Tension." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 329, no. 1 (August 1999): 305–12. http://dx.doi.org/10.1080/10587259908025951.

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7

de la Fuente, O. Rodríguez, M. A. González-Barrio, V. Navarro, B. M. Pabón, I. Palacio, and A. Mascaraque. "Surface defects and their influence on surface properties." Journal of Physics: Condensed Matter 25, no. 48 (November 7, 2013): 484008. http://dx.doi.org/10.1088/0953-8984/25/48/484008.

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8

Xiao, Xingcheng, Yang Tse Cheng, Brian W. Sheldon, and Janet Rankin. "Condensed water on superhydrophobic carbon films." Journal of Materials Research 23, no. 8 (August 2008): 2174–78. http://dx.doi.org/10.1557/jmr.2008.0260.

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Nanostructured carbon materials, including carbon nanotubes, nanofibers, and nanowalls, exhibit a wide range of interesting properties dictated by the many different bonding configurations. Many of these materials can possess superhydrophobic behavior when water drops are placed on their surfaces: these drops have high contact angles and can roll freely on the surfaces, which is desirable for self-cleaning. In this work, we prepared porous carbon films using a microwave plasma enhanced chemical vapor deposition technique. These films showed superhydrophobicity with contact angle of 150°, which was explained by the synergetic effect of the highly rough surface combined with the hydrogen terminated edges of graphene sheets. However, the condensed water drops can behave differently: the drops did not roll readily. This behavior mimicked that of water on lotus leaves and further demonstrated that the reported superhydrophobic behavior is a function of how the water gets on to the surfaces.
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9

Lai, W. S., Y. N. Osetsky, and D. J. Bacon. "Point-defect properties of and sputtering events in the {001} surfaces of Ni3Al I. Surface and point-defect properties." Philosophical Magazine 84, no. 2 (January 11, 2004): 173–91. http://dx.doi.org/10.1080/14786430310001623560.

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10

Shina, Hoon-Kyu, Jeong-Yeul Seo, Hyein Jeong, Burm-Jong Lee, and Young-Soo Kwona. "Electrical Properties and Surface Structure of Polyurethane Monolayers." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 370, no. 1 (October 2001): 395–98. http://dx.doi.org/10.1080/10587250108030114.

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11

López-Lozano, X., Cecilia Noguez, and L. Meza-Montes. "Optical properties of the cleavage InAs(110) surface." physica status solidi (c), no. 8 (December 2003): 2992–96. http://dx.doi.org/10.1002/pssc.200303842.

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12

Kim, Y. W. "Surface Position-Resolved Thermophysical Properties for Metallic Alloys." International Journal of Thermophysics 28, no. 2 (April 26, 2007): 732–41. http://dx.doi.org/10.1007/s10765-007-0171-5.

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13

Fedorenkova, L. I. "Structure and Properties of Multicomponent Surface Layers on Steel." METALLOFIZIKA I NOVEISHIE TEKHNOLOGII 42, no. 7 (September 18, 2020): 989–96. http://dx.doi.org/10.15407/mfint.42.07.0989.

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14

Sun, Jing-Bo, Jian-Gang Yao, Jiang Meng, Shuping Li, Yong Jiang, and Jigang Wang. "Surface energies and electronic properties of intermetallic compound B2-AgMg." Modern Physics Letters B 33, no. 08 (March 20, 2019): 1950097. http://dx.doi.org/10.1142/s0217984919500970.

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A new method was used to predict the surface energies of three low-index surfaces for intermetallic compound B2-AgMg. The results show that Ag-terminal and Mg-terminal are the two kinds of surface models for (1 0 0) and (1 1 1) surfaces which are non-stoichiometry. (1 1 0) surface has only one surface terminal, which is stoichiometry, and the smallest surface energy (about [Formula: see text] in three low-index surfaces. The surface energies are related to the chemical potential of Ag and Mg atoms for (1 0 0) and (1 1 1) surfaces, but it is of no concern to this factor for stoichiometry (1 1 0) surface. Analysis of electronic properties is coincident with the calculated surface energies.
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15

Li, Yinghong, Jian Wang, Cheng Wang, Zhiyong An, Shengli Hou, and Fei Xing. "Properties of surface arc discharge in a supersonic airflow." Plasma Sources Science and Technology 19, no. 2 (March 12, 2010): 025016. http://dx.doi.org/10.1088/0963-0252/19/2/025016.

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16

Abdul-Kader, A. M., Basma A. El-Badry, M. F. Zaki, Tarek M. Hegazy, and Hany M. Hashem. "Ion beam modification of surface properties of CR-39." Philosophical Magazine 90, no. 19 (July 7, 2010): 2543–55. http://dx.doi.org/10.1080/14786431003630728.

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17

Mochizuki, A., T. Makino, H. Shiroto, Y. Kiyota, and T. Yoshihara. "Surface Anchoring Influence on Polarization Switching Properties of Ssflcs." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 304, no. 1 (September 1997): 351–56. http://dx.doi.org/10.1080/10587259708046981.

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18

Joho, Felix, Pete Novák, Otto Haas, Alain Monnier, and Francis Fischer. "Influence of Graphite Surface Modifications on Lithium Intercalation Properties." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 310, no. 1 (February 1998): 383–88. http://dx.doi.org/10.1080/10587259808045366.

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19

Jiang, Hao, Suruchi Fialoke, Zachariah Vicars, and Amish J. Patel. "Correction: Characterizing surface wetting and interfacial properties using enhanced sampling (SWIPES)." Soft Matter 17, no. 14 (2021): 3976–77. http://dx.doi.org/10.1039/d1sm90055b.

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20

Śliwa, Izabela, and A. V. Zakharov. "Structural, Optical and Dynamic Properties of Thin Smectic Films." Crystals 10, no. 4 (April 20, 2020): 321. http://dx.doi.org/10.3390/cryst10040321.

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The problem of predicting structural and dynamic behavior associated with thin smectic films, both deposited on a solid surface or stretched over an opening, when the temperature is slowly increased above the bulk transition temperature towards either the nematic or isotropic phases, remains an interesting one in the physics of condensed matter. A useful route in studies of structural and optical properties of thin smectic films is provided by a combination of statistical–mechanical theories, hydrodynamics of liquid crystal phases, and optical and calorimetric techniques. We believe that this review shows some useful routes not only for the further examining of the validity of a theoretical description of thin smectic films, both deposited on a solid surface or stretched over an opening, but also for analyzing their structural, optical, and dynamic properties.
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21

Narhe, R., D. Beysens, and V. S. Nikolayev. "Dynamics of Drop Coalescence on a Surface: The Role of Initial Conditions and Surface Properties." International Journal of Thermophysics 26, no. 6 (November 2005): 1743–57. http://dx.doi.org/10.1007/s10765-005-8593-4.

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22

Jenks, Cynthia J., and Patricia A. Thiel. "Surface Properties of Quasicrystals." MRS Bulletin 22, no. 11 (November 1997): 55–58. http://dx.doi.org/10.1557/s0883769400034448.

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A variety of opportunities to develop technological applications of quasicrystals is being considered. Several of these are discussed in this issue. A common feature of many proposed applications is that they involve surface or near-surface interactions. Information about the surface structure, composition, and chemistry is prerequisite to understanding the origin of the desirable traits of quasicrystals. For instance, basic issues of surface structure—whether quasicrystals are intrinsically rough or flat, quasicrystalline or not quasicrystalline—impact directly on our understanding of their surface thermodynamic, electronic, and chemical properties.
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23

Yue, Chenxi, Shuye Jiang, Hao Zhu, Lin Chen, Qingqing Sun, and David Zhang. "Device Applications of Synthetic Topological Insulator Nanostructures." Electronics 7, no. 10 (October 1, 2018): 225. http://dx.doi.org/10.3390/electronics7100225.

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This review briefly describes the development of synthetic topological insulator materials in the application of advanced electronic devices. As a new class of quantum matter, topological insulators with insulating bulk and conducting surface states have attracted attention in more and more research fields other than condensed matter physics due to their intrinsic physical properties, which provides an excellent basis for novel nanoelectronic, optoelectronic, and spintronic device applications. In comparison to the mechanically exfoliated samples, the newly emerging topological insulator nanostructures prepared with various synthetical approaches are more intriguing because the conduction contribution of the surface states can be significantly enhanced due to the larger surface-to-volume ratio, better manifesting the unique properties of the gapless surface states. So far, these synthetic topological insulator nanostructures have been implemented in different electrically accessible device platforms via electrical, magnetic and optical characterizations for material investigations and device applications, which will be introduced in this review.
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24

KIKUCHI, SHOICHI, KENGO FUKAZAWA, JUN KOMOTORI, and MASAO SHIMIZU. "FATIGUE PROPERTIES OF HYBRID SURFACE MODIFIED SCM435H STEEL." International Journal of Modern Physics B 20, no. 25n27 (October 30, 2006): 3646–51. http://dx.doi.org/10.1142/s0217979206040131.

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In order to clarify the effects of nitriding and hybrid surface modification process combining nitriding and induction hardening on fatigue properties of SCM435H steel, high cycle fatigue tests were carried out with a rotational bending machine at room temperature. Observations of fracture surfaces and measurement of hardness and residual stress distributions were carried out to investigate the fracture mechanism. It was revealed that hybrid surface modification process generated a compressive residual stress field and hardened even at center of the specimen. Fatigue strength of hybrid surface modified specimens was much higher than that of substrate and nitrided specimens. This was because a transition of fracture mode from internal to surface fracture; fatigue fracture of nitrided specimens occurred at inside of the hardened layer, in the case of hybrid surface modified specimens, however, fatigue crack initiated at the surface of the specimen with higher hardness and higher compressive residual stress.
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25

Bodnar’, I. V., M. A. Osipova, V. Yu Rud’, Yu V. Rud’, and B. Kh Bairamov. "Photoelectric properties of In/CdP2 surface barrier structures." Journal of Applied Spectroscopy 77, no. 1 (March 2010): 148–51. http://dx.doi.org/10.1007/s10812-010-9307-7.

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26

Ahuja, R., A. K. Solanki, and S. Auluck. "Fermi Surface Properties of Platinum." physica status solidi (b) 168, no. 2 (December 1, 1991): 509–18. http://dx.doi.org/10.1002/pssb.2221680212.

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27

Ristein, J., F. Maier, M. Riedel, J. B. Cui, and L. Ley. "Surface Electronic Properties of Diamond." physica status solidi (a) 181, no. 1 (September 2000): 65–76. http://dx.doi.org/10.1002/1521-396x(200009)181:1<65::aid-pssa65>3.0.co;2-z.

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28

Kim, Sung-Mog, and Jong-Duk Kim. "Surface Properties of Rubbed Polyimide for Alignment of Liquid Crystal." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 287, no. 1 (August 1996): 229–37. http://dx.doi.org/10.1080/10587259608038758.

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29

Lee, Young-Jin, Hyun Jung Kwon, Su-An Choi, Young Keun Chang, Young H. Chang, and Jong-Duk Kim. "Surface Properties of Metallophthalocyanine LB Films and their Sensing Applications." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 337, no. 1 (November 1999): 501–4. http://dx.doi.org/10.1080/10587259908023487.

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30

Komitov, Lachezar, and Kunihiro Ichimura. "Photo-Induced Changes of Bulk and Surface Liquid Crystal Properties." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 360, no. 1 (April 2001): 161–91. http://dx.doi.org/10.1080/10587250108025705.

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31

Evans-Nguyen, Kenyon M., and Mark H. Schoenfisch. "Fibrin Proliferation at Model Surfaces: Influence of Surface Properties." Langmuir 21, no. 5 (March 2005): 1691–94. http://dx.doi.org/10.1021/la047303h.

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32

Arco, M. del, C. Martin, J. Mateos, and V. Rives. "Surface properties of Na-doped V2O5/TiO2systems." Journal of Physics: Condensed Matter 1, SB (October 1, 1989): SB235—SB236. http://dx.doi.org/10.1088/0953-8984/1/sb/056.

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33

Leyrer, J., B. Vielhaber, M. I. Zaki, Shuxian Zhuang, J. Weitkamp, and H. Knözinger. "Structure and surface properties of supported oxides." Materials Chemistry and Physics 13, no. 3-4 (September 1985): 301–14. http://dx.doi.org/10.1016/0254-0584(85)90061-6.

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34

Yücel, Melike Behiye. "Coupling of Photonic Crystal Surface Modes." Advances in Condensed Matter Physics 2022 (August 10, 2022): 1–9. http://dx.doi.org/10.1155/2022/8947410.

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Guiding and evanescent coupling properties of surface modes bound to the interfaces of two-dimensional photonic crystals in close proximity are numerically demonstrated. Interacting photonic crystals are composed of silicon pillars in air, where their outermost layers facing each other are annular. Surface modes are identified through supercell band structure computations, while their excitation by the electromagnetic waves through a perpendicular insertion waveguide is demonstrated using finite-difference time-domain simulations. Lifting the degeneracy between the surface modes as a consequence of bringing two identical photonic crystal surfaces to a sufficient distance results in evanescent coupling in a beating manner whose beat length linearly varies between 10 and 20 periods up to a frequency at which both surface modes travel with the same group velocity. The surface mode coupling phenomenon could be employed either to enhance sensitivity or to reduce device size in bio/chemical sensor applications since the effective travelling length of surface waves increases by about 3.5 times due to evanescent coupling.
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35

Tian, Shouceng, Tianyu Wang, Gensheng Li, Mao Sheng, and Panpan Zhang. "Nanoscale Surface Properties of Organic Matter and Clay Minerals in Shale." Langmuir 35, no. 17 (March 28, 2019): 5711–18. http://dx.doi.org/10.1021/acs.langmuir.9b00157.

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36

Fung, A. K., A. J. Blanchard, and M. F. Chen. "Polarization Properties in Random Surface Scattering." Progress In Electromagnetics Research 03 (1990): 143–235. http://dx.doi.org/10.2528/pier89082700.

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37

Adachi, Masatoshi, Tomoakj Karaki, and Wataru Miyamoto. "Surface acoustic wave properties of La3Ga5SiO14crystals." Ferroelectrics 229, no. 1 (May 1999): 159–64. http://dx.doi.org/10.1080/00150199908224333.

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38

Matsuda, Tatsuma D., Nguyen Duc Dung, Yoshinori Haga, Shugo Ikeda, Etsuji Yamamoto, Tatsuro Ishikura, Toyoaki Endo, Tetsuya Takeuchi, Rikio Settai, and Yoshichika Ōnuki. "Fermi surface properties of YbCu2 Si2." physica status solidi (b) 247, no. 3 (February 8, 2010): 757–59. http://dx.doi.org/10.1002/pssb.200983027.

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39

Cavallotti, P., D. Colombo, P. d'Arcangelo, and G. Greppi. "Surface properties of hard magnetic powders." Journal of Magnetism and Magnetic Materials 54-57 (February 1986): 1636–38. http://dx.doi.org/10.1016/0304-8853(86)90956-x.

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40

MacLaren, J. M., S. Crampin, D. D. Vvedensky, and J. B. Pendry. "Layer Korringa-Kohn-Rostoker technique for surface and interface electronic properties." Physical Review B 40, no. 18 (December 15, 1989): 12164–75. http://dx.doi.org/10.1103/physrevb.40.12164.

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41

Fu, Yangyang, Peng Zhang, John P. Verboncoeur, Andrew J. Christlieb, and Xinxin Wang. "Effect of surface protrusion on plasma sheath properties in atmospheric microdischarges." Physics of Plasmas 25, no. 1 (January 2018): 013530. http://dx.doi.org/10.1063/1.5011768.

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42

Shcherbanev, S. A., Ch Ding, S. M. Starikovskaia, and N. A. Popov. "Filamentary nanosecond surface dielectric barrier discharge. Plasma properties in the filaments." Plasma Sources Science and Technology 28, no. 6 (June 25, 2019): 065013. http://dx.doi.org/10.1088/1361-6595/ab2230.

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43

Papazian, H. A. "Correlation of surface tension with bulk properties for molten alkali halides." International Journal of Thermophysics 6, no. 5 (September 1985): 533–37. http://dx.doi.org/10.1007/bf00508895.

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44

Ancilotto, Francesco, and Flavio Toigo. "Properties of an electron bubble approaching the surface of liquid helium." Physical Review B 50, no. 17 (November 1, 1994): 12820–30. http://dx.doi.org/10.1103/physrevb.50.12820.

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45

Khasawneh, Khaleel, Hongli Liu, and Chunpei Cai. "Surface properties for rarefied circular jet impingement on a flat plate." Physics of Fluids 23, no. 2 (February 2011): 027102. http://dx.doi.org/10.1063/1.3549934.

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46

Habermeier, H. U. "Substrate surface engineering for tailoring properties of functional ceramic thin films." physica status solidi (c) 1, no. 7 (May 2004): 1614–19. http://dx.doi.org/10.1002/pssc.200304427.

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47

Hogan, Conor, Rita Magri, and Rodolfo Del Sole. "Structure and optical properties of the Sb-stabilized GaSb(001) surface." physica status solidi (c) 7, no. 2 (February 2010): 177–80. http://dx.doi.org/10.1002/pssc.200982499.

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48

ZUBOV, V. I., I. V. MAMONTOV, and N. P. TRETYAKOV. "THE MICROSCOPIC THEORY OF THE SURFACE PROPERTIES OF ANHARMONIC CRYSTALS I: General Method and (001) Surface of BCC Crystal." International Journal of Modern Physics B 06, no. 02 (January 20, 1992): 197–219. http://dx.doi.org/10.1142/s0217979292000116.

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The self-consistent theory of the structural, dynamical, and thermodynamic surface properties of anharmonic crystals previously given for one- and two-dimensional models is extended to the surfaces of three-dimensional crystals which take into account the surface anisotropy. After considering the reference system, in the general case, the equations for the properties of the interface cyrstal-vapour to the second order in the temperature are derived. The (001) face of the BCC crystal is investigated. The lattice relaxation and dynamics are calculated. The surface Helmholtz free energy and other thermodynamic properties are obtained. At high temperatures, the surface specific heat increases linearly with temperature due to the anharmonicity.
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49

Tran, Thien, Xiaoyi Chen, Sarthak Doshi, Christopher M. Stafford, and Haiqing Lin. "Grafting polysiloxane onto ultrafiltration membranes to optimize surface energy and mitigate fouling." Soft Matter 16, no. 21 (2020): 5044–53. http://dx.doi.org/10.1039/d0sm00551g.

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50

Rousière, O., D. Lemoine, A. Quémerais, C. K. Assi, R. Granger, and R. Triboulet. "Surface properties of passivated." Semiconductor Science and Technology 13, no. 6 (June 1, 1998): 622–29. http://dx.doi.org/10.1088/0268-1242/13/6/014.

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