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1

Camus, Hubert. "Evolution des reseaux hydrographiques au contact Cevennes-Grands Causses meridionaux; consequences sur l'evaluation de la surrection tectonique." Bulletin de la Société Géologique de France 172, no. 5 (September 1, 2001): 549–62. http://dx.doi.org/10.2113/172.5.549.

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Анотація:
Abstract The Mediterranean catchment of the Cevennes (S. France) presents deep incision of the river network (fig. 1 and 2). Combined geomorphology and analyses of the residual sedimentary formations allows to reconstruct a complex history of river network evolution, including capture of tributaries of the Herault River (fig. 1, 2 and 3). The history of uplift of the upstream drainage area could be estimated from the provenance studies of the fluvial and karstic deposits, however river incision is also controlled sea-level changes and differential erosion, which makes reconstruction more complex. Allochthonous clasts types: Analyses of allochthonous deposits on the Grands Causses surface reveals different origin for sediments from the hill top and the Airoles valley (fig. 4 b), which was previously unrecognised. Facies 1 is found on the highest points of the Grands Causses surface (well sorted rounded quartz pebbles in red shale matrix) it corresponds to a weathered residual sediments (dismantling of an ancient cover). Facies 2 is found on the slope of the Airoles Valley (fig. 7). It consists of alluvial crystalline poorly sorted clasts with outsized clasts (up to 50 cm) of quartz-vein, schists in a matrix of shales and sand (weathered granite). Between the hill tops and the Airoles Valley, karstic network presents a sediment fill with clasts reworked from facies 1 and facies 2 (fig. 6). Airoles valley model; an example of diachronic formation of drainage network: The Airoles dry valley stretches on the Grands Causses from the north (700 m) to the south into the present thalweg line of the Vis canyon (500 m) (fig. 1b & 3). Crystalline deposits witness an ancient catchment in the Cevennes. Presently, the catchment in the crystalline basement is disconnected and captured by the Arre River flowing eastwards (fig. 3 & 4a). The profile of the Airoles abandoned valley connects with the present Vis Canyon, therefore, at the time of capture, incision of the Vis canyon had reached its present altitude (fig. 4a). The geomorphologic evolution of this area took place in three stages (fig. 8). 1) The Grands Causses acted as piedmont for the crystalline highlands of the Massif Central (fig. 8A). A latter karstic evolution (tropical climate) allowed the weathered residual sediments (facies 1) (fig. 8A). 2) Incision of the Vis karstic canyon implies that the Herault incision and terraces (facies 2) (fig. 8B) of the Airoles valley occurred during this stage. 3) The Arre valley head propagates westward by regressive erosion and finally captured the Airoles river crystalline catchment (fig. 8C). Consequence for the Cevennes uplift and hydrographic network development: Although the values of present vertical incision in the Vis canyon and in the Arre valley are similar, but they achieved at different time. In addition, the narrow and deep canyon of the Vis is due to vertical incision from the karstic surface of the Grands Causses, whereas the Arre wide valley results from (a younger) lateral slopes retreat from a low Herault base-level. The Vis karstic canyon developed in a similar way to the major karstic canyons of both Mediterranean and Atlantic catchment (i.e. Tarn). This rules out a Messinian Mediterranean desiccation as incision driving mechanism and suggests tectonic uplift of the Cevennes and surrounding areas. The Tarn being already incised by 13 My [Ambert, 1990], it implies a Miocene age for the incision. Conclusion: The amplitude of the vertical incision cannot therefore be used in a simple way to interpret the uplift history of the basement. Consequently, geomorphologic analysis appears to be a prerequisite to distinguish the part played by each factor, and to select the site of uplift measurement.
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2

Serrate, Bénédicte. "Reseaux de conception innovante et formes de proximites." Revista Eletrônica de Estratégia & Negócios 1, no. 2 (August 24, 2010): 103. http://dx.doi.org/10.19177/reen.v1e22008103-118.

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La conception, appelée « design » dans les entreprises industrielles, représente dans le processus d’innovation une étape essentielle pourtant peu étudiée encore par les économistes. Elle mobilise pour aboutir à des innovations de plus en plus jugées essentielles à la compétitivité de l’entreprise, quantité d’acteurs internes et externes selon une logique de réseau sans cesse renouvelée. A partir de l’observation de cas empiriques, nous avons tenté dans cet article de comprendre comment s’organisaient ces réseaux innovants. Aujourd’hui dans la plupart des pays qui pratiquent des politiques de développement économique local, il semble établi qu’il faille construire des proximités géographiques entre acteurs pour que se développent des relations industrielles favorisant la dynamique d’innovation et le transfert des connaissances. L’abondance des « clusters » et des « pôles de compétitivité » partout dans le monde témoigne de ce postulat. En analysant les modes d’organisation des réseaux de conception nous avons donc cherché à vérifier si la proximité géographique constituait encore un ressort essentiel et si la globalisation des entreprises ne laissait pas apparaitre d’autres formes de proximités.
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3

Zhang, Jian Li, and Yan Min Li. "Reseach on Secondary Cooling Dynamic Control Model in Continuous Casting of Slabs." Advanced Materials Research 268-270 (July 2011): 1152–56. http://dx.doi.org/10.4028/www.scientific.net/amr.268-270.1152.

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one improved finite volume method is proposed, expatiating on the basic idea and integrating the partial derivative equation for the secondary spary water dynamic cooling control model. The semi-discrete equation for derivative of time is obtained.Combinating with an introducted slab continuous casting production line in some steel mill, according to the Q235 actual parameters, what is obtained is surface temperature distribution, the changing of surface temperature and the water flow rate because of the varying of casting speed. The results of simulations performed using the mathematical model are validated against the measured values and a good agreement is observed, Verifing the validity of the model.The model occupies less computer memory, solving simple
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4

Combe, N., J. R. Huntzinger, and J. Morillo. "Surface loving and surface avoiding modes." European Physical Journal B 68, no. 1 (February 21, 2009): 47–58. http://dx.doi.org/10.1140/epjb/e2009-00061-3.

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5

Kivshar, Yuri S., Fei Zhang, and Shozo Takeno. "Multistable nonlinear surface modes." Physica D: Nonlinear Phenomena 119, no. 1-2 (August 1998): 125–33. http://dx.doi.org/10.1016/s0167-2789(98)00071-2.

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6

Gernoth, K. A., J. W. Clark, G. Senger, and M. L. Ristig. "Surface modes of liquidHe4." Physical Review B 49, no. 22 (June 1, 1994): 15836–48. http://dx.doi.org/10.1103/physrevb.49.15836.

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7

Zhang, T. H., X. K. Ren, B. H. Wang, Z. J. Hu, W. W. Shao, J. Yang, H. Z. Kang, et al. "Modes of photorefractive surface waves." Journal of Modern Optics 54, no. 10 (July 10, 2007): 1445–52. http://dx.doi.org/10.1080/09500340601156785.

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8

Hesse, D., and P. Cawley. "Surface wave modes in rails." Journal of the Acoustical Society of America 120, no. 2 (August 2006): 733–40. http://dx.doi.org/10.1121/1.2211587.

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9

Puri, A., and W. L. Schaich. "Surface modes in accumulation layers." Physical Review B 31, no. 2 (January 15, 1985): 974–80. http://dx.doi.org/10.1103/physrevb.31.974.

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10

Gorentsveig, V. I., Yu S. Kivshar, A. M. Kosevich, and E. S. Syrkin. "Nonlinear surface modes in crystals." International Journal of Engineering Science 29, no. 3 (January 1991): 271–79. http://dx.doi.org/10.1016/0020-7225(91)90144-r.

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11

Thorpe, M. F. "Bulk and surface floppy modes." Journal of Non-Crystalline Solids 182, no. 1-2 (March 1995): 135–42. http://dx.doi.org/10.1016/0022-3093(94)00545-1.

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12

Kaffel, A., and M. Renardy. "Surface modes in inviscid free surface shear flows." ZAMM - Journal of Applied Mathematics and Mechanics / Zeitschrift für Angewandte Mathematik und Mechanik 91, no. 8 (April 26, 2011): 649–52. http://dx.doi.org/10.1002/zamm.201000165.

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13

Weston, David E., Michael L. Somers, and Jack Revie. "GLORIA interference patterns with modes akin to surface-duct modes." Journal of the Acoustical Society of America 89, no. 5 (May 1991): 2180–84. http://dx.doi.org/10.1121/1.400911.

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14

Rudik, A. V., and G. V. Pasov. "DEPENDENCE OF CUTTING SURFACE PARAMETERS FROM SURFACE GRINDING MODES." Scientific notes of Taurida National V.I. Vernadsky University. Series: Technical Sciences 4, no. 1 (2019): 7–11. http://dx.doi.org/10.32838/2663-5941/2019.4-1/02.

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15

Reinecke, T. L., and S. C. Ying. "Surface modes of the clean reconstructed W(100) surface." Physical Review B 48, no. 8 (August 15, 1993): 5679–81. http://dx.doi.org/10.1103/physrevb.48.5679.

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16

Rezzouk, Yamina, Madiha Amrani, Soufyane Khattou, El Houssaine El Boudouti, and Bahram Djafari-Rouhani. "Surface modes in plasmonic stubbed structures." Materials Today: Proceedings 45 (2021): 7752–55. http://dx.doi.org/10.1016/j.matpr.2021.03.438.

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17

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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18

JIANG ZUI-MIN and WU ZI-QIN. "SURFACE VIBRATION MODES OF Si(111)." Acta Physica Sinica 37, no. 4 (1988): 629. http://dx.doi.org/10.7498/aps.37.629.

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19

Rakhimyanov, A. Kh, Yu S. Semenova, and A. A. Zhivaga. ""TECHNOLOGICAL MODES FOR ULTRASONIC SURFACE HARDENING." Vestnik of Kuzbass State Technical University 18, no. 2 (2018): 84–92. http://dx.doi.org/10.26730/1999-4125-2018-2-84-92.

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20

Morozov, N. F., and P. E. Tovstik. "On the modes of surface stability." Doklady Physics 56, no. 5 (May 2011): 300–304. http://dx.doi.org/10.1134/s1028335811050107.

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21

Moch, Philippe, Jean-Pierre Jardin, and Vladimir Dvořák. "Surface modes in a ferroelectric film." Ferroelectrics 241, no. 1 (March 2000): 141–48. http://dx.doi.org/10.1080/00150190008224985.

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22

SANTOS, A. R. DOS, and F. A. OLIVEIRA. "SURFACE MODES IN SEMI-INFINITE FERROELECTRICS." Modern Physics Letters B 01, no. 07n08 (November 1987): 271–73. http://dx.doi.org/10.1142/s0217984987000399.

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23

Inoue, Masahiro. "Optical bistability by surface resonance modes." Physical Review Letters 58, no. 9 (March 2, 1987): 871–73. http://dx.doi.org/10.1103/physrevlett.58.871.

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24

Manson, J. R. "Atom scattering from surface Einstein modes." Physical Review B 37, no. 12 (April 15, 1988): 6750–56. http://dx.doi.org/10.1103/physrevb.37.6750.

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25

Sahoo, Prasana, S. Dhara, S. Dash, A. K. Tyagi, Baldev Raj, C. R. Das, P. Chandramohan, and M. P. Srinivasan. "Surface optical modes in GaN nanowires." International Journal of Nanotechnology 7, no. 9/10/11/12 (2010): 823. http://dx.doi.org/10.1504/ijnt.2010.034690.

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26

Martinos, S. S. "Surface electromagnetic modes in metal spheres." Physical Review B 31, no. 4 (February 15, 1985): 2029–32. http://dx.doi.org/10.1103/physrevb.31.2029.

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27

Onodera, Y., and P. K. Choi. "Surface-wave modes on soft gels." Journal of the Acoustical Society of America 104, no. 6 (December 1998): 3358–63. http://dx.doi.org/10.1121/1.423919.

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28

Pleiner, H., J. L. Harden, and P. Pincus. "Surface Modes on a Viscoelastic Medium." Europhysics Letters (EPL) 7, no. 5 (November 1, 1988): 383–87. http://dx.doi.org/10.1209/0295-5075/7/5/001.

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29

Zalutskaya, A. A., and A. V. Prokaznikov. "Edge modes splitting by nanostructured surface." Journal of Physics: Conference Series 541 (October 27, 2014): 012079. http://dx.doi.org/10.1088/1742-6596/541/1/012079.

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30

MIMS, C., N. BAYANI, A. JACOBSON, and P. VANDERHEIDE. "Modes of surface exchange in LaSrCrFeO." Solid State Ionics 176, no. 3-4 (January 31, 2005): 319–23. http://dx.doi.org/10.1016/j.ssi.2004.08.014.

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31

Schmidt, F. P., H. Ditlbacher, U. Hohenester, A. Hohenau, F. Hofer, and J. R. Krenn. "Universal Scaling of Surface Plasmon Modes." Microscopy and Microanalysis 20, S3 (August 2014): 624–25. http://dx.doi.org/10.1017/s143192761400484x.

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32

Snyder, A. W., and H. T. Tran. "Surface modes of power law nonlinearities." Optics Communications 98, no. 4-6 (May 1993): 309–12. http://dx.doi.org/10.1016/0030-4018(93)90201-f.

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33

Larraza, A., and M. B. Walker. "Surface-phason modes in incommensurate crystals." Physical Review B 40, no. 2 (July 15, 1989): 977–79. http://dx.doi.org/10.1103/physrevb.40.977.

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34

Fischer, Hans Peter, Philipp Maass, and Wolfgang Dieterich. "Novel Surface Modes in Spinodal Decomposition." Physical Review Letters 79, no. 5 (August 4, 1997): 893–96. http://dx.doi.org/10.1103/physrevlett.79.893.

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35

Narayanaswamy, Arvind, and Gang Chen. "Surface modes for near field thermophotovoltaics." Applied Physics Letters 82, no. 20 (May 19, 2003): 3544–46. http://dx.doi.org/10.1063/1.1575936.

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36

Nkoma, John S. "Surface modes of coupled sphere systems." Solid State Communications 78, no. 6 (May 1991): 525–29. http://dx.doi.org/10.1016/0038-1098(91)90369-7.

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37

Nkoma, John S. "Surface modes of a composite medium." Solid State Communications 87, no. 3 (July 1993): 241–44. http://dx.doi.org/10.1016/0038-1098(93)90484-5.

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38

Gorentsveig, V. I., Yu S. Kivshar, A. M. Kosevich, and E. S. Syrkin. "Nonlinear surface elastic modes in crystals." Physics Letters A 144, no. 8-9 (March 1990): 479–86. http://dx.doi.org/10.1016/0375-9601(90)90519-t.

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39

Tang, Tingting. "Generation of Guiding Modes by Surface Modes in Anisotropic Metamaterial Waveguide." IEEE Photonics Technology Letters 25, no. 18 (September 2013): 1781–84. http://dx.doi.org/10.1109/lpt.2013.2273454.

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40

Lavoie, Benjamin R., Patrick M. Leung, and Barry C. Sanders. "Low-loss surface modes and lossy hybrid modes in metamaterial waveguides." Photonics and Nanostructures - Fundamentals and Applications 10, no. 4 (October 2012): 602–14. http://dx.doi.org/10.1016/j.photonics.2012.05.010.

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41

Xu, Jun Jun, Hao Chi Zhang, Qian Zhang, and Tie Jun Cui. "Efficient conversion of surface-plasmon-like modes to spatial radiated modes." Applied Physics Letters 106, no. 2 (January 12, 2015): 021102. http://dx.doi.org/10.1063/1.4905580.

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42

Feshchenko, R. Yu, O. O. Erokhina, R. N. Eremin, and B. E. Matylskiy. "Analysis of methods for increasing the oxidation resistance of carbon-graphite products used in metallurgical and chemical units." Proceedings of Irkutsk State Technical University 25, no. 3 (July 6, 2021): 380–90. http://dx.doi.org/10.21285/1814-3520-2021-3-380-390.

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Анотація:
This review study analyses the existing methods for increasing the oxidation resistance of carbon-graphite products, as well as assesses their applicability in metallurgical and chemical units. The reseach basis was the data published on the oxidation mechanism of carbon-graphite materials, conditions for their use in metallurgical and chemical processes, as well as existing technologies aimed at improving the oxidation resistance of artificial graphites. The existing ideas about the kinetics of carbon graphite oxidation are described depending on temperature conditions. A review of existing technologies for increasing the oxidation resistance of materials and their economic efficiency, taking into account the conditions of their operation, was carried out. Prospects of the presented solutions for the units of metallurgical and chemical industries were analysed. Three modes of oxidation of graphitised materials were distinguished on the basis of operating conditions, chemical and physical properties. According to this classification, the most rational method for increasing oxidation resistance consists in the impregnation of carbon-graphite materials with the formation of a protective glassy coating in the volume of through pores or with the formation of a coating (a continuous layer on the surface of the product) due to the occurrence of a chemical reaction with the reagents used. For most metallurgical and chemical units, the impregnation of carbon-graphite materials with the formation of borate and phosphate glasses is preferable, primarily due to lower economic costs. The applicability of this method is currently limited by temperature conditions, at which the protective properties and continuity of the formed glassy coatings are preserved. Therefore, additional research is required to adapt the conventional technological and technical solutions to the high-temperature conditions of metallurgical units (over 800°C).
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43

INO, S. "SURFACE STRUCTURES AND SURFACE CONDUCTANCE DURING METAL ADSORPTION ON SEMICONDUCTORS." Surface Review and Letters 04, no. 05 (October 1997): 969–75. http://dx.doi.org/10.1142/s0218625x97001140.

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Epitaxial growth modes for "two-step deposition" processes of metals on a Si(111) surface were investigated. Depth distributions of composition during the growth were analyzed by using RHEED-TRAXS (total reflection angle X-ray spectroscopy). We first made [Formula: see text]-(Ag, Au, Ga), [Formula: see text]-Sn and (4×1)-In structures, and then second metals (Ag, Au, Sn, Ga and In) were deposited on these surfaces at room temperature. Growth processes observed are classified into five growth modes: ordinary growth (O), alloying growth (A), substitution atom growth (S), particle formation growth mode (P) and floating atom growth (F). During the growth processes, we measured also surface conductivities which showed interesting behaviors. These results can be partly understood considering the growth modes, atomic arrangement, surface composition, Fermi level pinning and band bending, etc.
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44

YANG, FUZI, G. W. BRADBERRY, and J. R. SAMBLES. "LONG RANGE SURFACE EXCITON POLARITONS: NEW LONG RANGE SURFACE MODES." Modern Physics Letters B 04, no. 18 (October 10, 1990): 1119–32. http://dx.doi.org/10.1142/s0217984990001410.

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The work on the recently discovered long range coupled surface mode, the long range surface exciton-polariton is reviewed. The basic simple analytic equations which describe its dispersion in the symmetric case are presented and discussed. Adding a coupling prism perturbs these equations but does not necessarily lead automatically to a broader resonance. It is shown how 100% coupling is achieved for the symmetrically surrounded layer by a coupling gap thickness which makes the resonance lie very close to the critical angle. The consequences of small changes of symmetry and a small amount of absorption in the surrounding dielectrics are discussed.
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45

Cao, B. H., M. W. Kim, H. Schaffer, and H. Z. Cummins. "Surface modes on polymer solutions by surface light‐scattering techniques." Journal of Chemical Physics 95, no. 12 (December 15, 1991): 9317–21. http://dx.doi.org/10.1063/1.461160.

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46

Andres, M. V., and V. Such. "Cylindrical surface waveguide modes using a surface impedance dyadic method." IEE Proceedings H Microwaves, Antennas and Propagation 134, no. 2 (1987): 130. http://dx.doi.org/10.1049/ip-h-2.1987.0026.

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