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Online since: January 2014
Authors: Feng Xia Qiu
The degree of a node (equation 1) (in this paper, the number of partners)is simply the number of other nodes connected directly to the node.
Thus, the degree centrality of node pk is given by: CD(PK)=iaij (Pi, PK ) (1) a Pi, PK =1, if node Pi and node PK are connected. a Pi, PK =0 otherwise.
During the four stages, the firm- research institute sub-network has 45, 76, 261 and 479 nodes respectively, averagely one firm has 1.2, 1.1, 1.3 and 1.4 research institutions partner and research institute has 1.1, 1.4, 1.8 and 2 firm partners.
As for the university-research institute sub-networks, during the first and second stage, there are 30 and 53 nodes apart, one research institute has only 1 and 1.5 university partner(s) respectively, and one university owns 1 and 2.3 research institute partner(s).
References [1] Joaqui´n M.
Thus, the degree centrality of node pk is given by: CD(PK)=iaij (Pi, PK ) (1) a Pi, PK =1, if node Pi and node PK are connected. a Pi, PK =0 otherwise.
During the four stages, the firm- research institute sub-network has 45, 76, 261 and 479 nodes respectively, averagely one firm has 1.2, 1.1, 1.3 and 1.4 research institutions partner and research institute has 1.1, 1.4, 1.8 and 2 firm partners.
As for the university-research institute sub-networks, during the first and second stage, there are 30 and 53 nodes apart, one research institute has only 1 and 1.5 university partner(s) respectively, and one university owns 1 and 2.3 research institute partner(s).
References [1] Joaqui´n M.
Online since: December 2013
Authors: Alexander F. Sharovarnikov, Dmitriy A. Korol’chenko
The scheme of the model space and the characteristic time of quenching is shown in Fig. 1.
Fig.1.
Determination of position of a plane of equal pressure (PEP) in a room with a steady burning before the extinguishing gas composition. 3.1.1.
References: [1] D’yakonov G.K.
The mathematical theory of combustion and explosion. - Moscow: Science, page-479, (1980)
Fig.1.
Determination of position of a plane of equal pressure (PEP) in a room with a steady burning before the extinguishing gas composition. 3.1.1.
References: [1] D’yakonov G.K.
The mathematical theory of combustion and explosion. - Moscow: Science, page-479, (1980)
Online since: March 2015
Authors: Yu Zhou, Qi Long Zhao, Min Wang
Generally speaking, scaffolds made by the hybrid technique maintained the nanofibrous structure (Fig.1), which was similar to that of scaffolds produced by conventional electrospinning.
Generally, these scaffolds also showed more loosely packed structures except for scaffolds made from the 30% PCL solution using mixed solvent of chloroform and DMF (9:1).
Fig.1 Morphology of the scaffolds Fig. 1(a) and (b) show the scaffolds made from 15% PCL solutions using mixed solvent of DCM and DMF (7: 3); Fig.1(c) and (d) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (7: 3); Fig 1(e) and (f) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (8: 2); and Fig. 1(g) and (h) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (9: 1).
References [1] R.
Spine J. 17(2008) 467-479
Generally, these scaffolds also showed more loosely packed structures except for scaffolds made from the 30% PCL solution using mixed solvent of chloroform and DMF (9:1).
Fig.1 Morphology of the scaffolds Fig. 1(a) and (b) show the scaffolds made from 15% PCL solutions using mixed solvent of DCM and DMF (7: 3); Fig.1(c) and (d) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (7: 3); Fig 1(e) and (f) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (8: 2); and Fig. 1(g) and (h) show the scaffolds made from 30% PCL solutions using mixed solvent of chloroform and DMF (9: 1).
References [1] R.
Spine J. 17(2008) 467-479
Online since: May 2013
Authors: Ze Fei Wei, Zi Yuan Yu, Xing Hua Zheng
However, drilling always causes tiny burrs along the edge of the holes [1].
Fig. 1 shows the theoretical scheme of ECD.
Table 1 shows the experimental parameters.
References [1] M.M.
Vol. 220(2006) 479-487.
Fig. 1 shows the theoretical scheme of ECD.
Table 1 shows the experimental parameters.
References [1] M.M.
Vol. 220(2006) 479-487.
Online since: September 2010
Authors: Han Huang, Rudy Irwan, Zhen Yu Zhang
Fig. 1 shows the SEM micrographs of Cd0.96Zn0.04Te (111)
wafer after wire sawing.
Fig. 1(b) shows the surface characteristics of being 'sticky' of soft materials after sawing.
Fig. 1(c) shows the feature of removal via cleavage, which has normal fracture feature.
References [1] T.E.
A Vol. 479 (2008), p. 373-379
Fig. 1(b) shows the surface characteristics of being 'sticky' of soft materials after sawing.
Fig. 1(c) shows the feature of removal via cleavage, which has normal fracture feature.
References [1] T.E.
A Vol. 479 (2008), p. 373-379
Online since: October 2011
Authors: Xue Mei Huang, Wei Hong Liu, Hong Quan Wang
For example, we sought only the three neighbors of a cube in Case-3 in [1], but we needed seek all six neighbors of a cube in Case-10 in [1].
Fig.1.
The flag value was set to 1.
References [1] W.
Reconstruction of the human cerebral cortex from MRI, IEEE Trans.on Medical Imaging, 1999,18(6): 467-479
Fig.1.
The flag value was set to 1.
References [1] W.
Reconstruction of the human cerebral cortex from MRI, IEEE Trans.on Medical Imaging, 1999,18(6): 467-479
Online since: March 2007
Authors: Hidehiro Onodera, Masato Shimono
Icosahedral Order in Supercooled Liquids and Glassy Alloys
Masato Shimonoa and Hidehiro Onoderab
National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, 305-0047 Japan
a
e-mail: shimono.masato@nims.go.jp
b
e-mail: onodera.hidehiro@nims.go.jp
Keywords: metallic glasses; supercooled liquid; computer simulation; rapid solidification
Abstract.
In other words, we assume that rAA = 1, rBB = 0.8, rAB = (rAA + rBB)/2 = 0.9, and eAA = eBB = eAB = 1.
The upper part of Fig. 2 shows the temperature dependence of the number Nico of the icosahedral clusters in the A40B60 system during the slowly quenched procedure (2×10 −4) shown by the closed triangles in Fig. 1.
References [1] A.
A 319 (1970) 479-493
In other words, we assume that rAA = 1, rBB = 0.8, rAB = (rAA + rBB)/2 = 0.9, and eAA = eBB = eAB = 1.
The upper part of Fig. 2 shows the temperature dependence of the number Nico of the icosahedral clusters in the A40B60 system during the slowly quenched procedure (2×10 −4) shown by the closed triangles in Fig. 1.
References [1] A.
A 319 (1970) 479-493
Online since: September 2007
Authors: Lars Nyborg, Yu Cao, S. Alfonso Pérez-García
Cao
1, a
, S.A.
Pérez-García 1, b and L.
The layered structure is inclined to form when the vanadium group metals (V, Nb and Ta) react thermally with SiC at high temperatures [3]. 60 80 100 120 800 o C, 1 o 950 o C, 1 o 2ϑ ( o ) Ta5Si3 Ta2C Ta Intensity 950 o C, 3 o 650 o C, 1 o Fig. 1.
References [1] I.P.
Lampert: Thin Solid Films Vol. 479 (2005), p. 59
Pérez-García 1, b and L.
The layered structure is inclined to form when the vanadium group metals (V, Nb and Ta) react thermally with SiC at high temperatures [3]. 60 80 100 120 800 o C, 1 o 950 o C, 1 o 2ϑ ( o ) Ta5Si3 Ta2C Ta Intensity 950 o C, 3 o 650 o C, 1 o Fig. 1.
References [1] I.P.
Lampert: Thin Solid Films Vol. 479 (2005), p. 59
Online since: January 2009
Authors: Jerzy Lis, Stanisława Jonas, Andrzej Koleżyński, Katarzyna Tkacz-Śmiech, Pawel Stoch
Model Studies of Microstructure Changes in Sintering of Ceramics
Stanisława Jonas1, Andrzej Koleżyński1, Jerzy Lis, Paweł Stoch
1
and Katarzyna Tkacz-Śmiech1, a
1
AGH University of Science and Technology, Faculty of Materials Science and Ceramics
Al.
The safety margin is assumed at the level of 1/10 of the radius.
The unknown powder packing is calculated as the limit of ρ at N-1/3 → 0.
Fig. 1.
A 319 (1970) 479 [11] K.
The safety margin is assumed at the level of 1/10 of the radius.
The unknown powder packing is calculated as the limit of ρ at N-1/3 → 0.
Fig. 1.
A 319 (1970) 479 [11] K.
Online since: April 2007
Authors: Ya Ru Zhang, Bo Ping Zhang, Yan Dong, Jing Feng Li
Effect of Ti Content on Microstructure and Dielectric Properties of Li
and Ti Co-doped NiO Thin Films
Ya-Ru Zhang1, Bo-Ping Zhang
1*
, Yan Dong
1 and Jing-Feng Li2
1
School of Materials Science and Engineering, University of Science and Technology Beijing,
100083, P.R.
References [1] B.G.
Forum Vol. 89 (2002) 217601-1
Forum Vol. 475-479 (2005), pp. 1595-1598
Forum Vol. 37 (1993), pp. 1
References [1] B.G.
Forum Vol. 89 (2002) 217601-1
Forum Vol. 475-479 (2005), pp. 1595-1598
Forum Vol. 37 (1993), pp. 1