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Jeong 1, a, J.B.
The tensile tests were carried out at an initial strain rate of 5x10 -3 s-1 and at room temperature.
Table 1.
References [1] T.
Kim : Materials Science Forum Vols. 475-479 (2005), p. 549 [7] T.

Analysis the Actual Nanostructure of a Phase Polyoctylfluorene Thin Film via Synchrotron Grazing-incidence X-ray Diffraction CHEN Liu-Ran 1, a, CHEN Xi 2,b, LIANG Ji-Cai 1,b and ZHANG Ji-Dong 2,d,* 1 College of Materials Science and Engineering, Jilin University, Changchun , 130022, P.R.China 2 State Key Lab of Polymer Physics and Chemistry, Changchun Institute of Applied Chemistry, Chinese Academy of Science, Changchun, 130022, P.R.China achenlr10@mails.jlu.edu.cn, bchenxi@ciac.jl.cn, c liang_jicai@yahoo.com.cn, djdzhang@ciac.jl.cn Keywords: polyoctylfluorene, actual nanostructure, grazing incidence X-ray diffraction.
Fig.1 shows the UV-Vis absorption spectra and photoluminescence spectra of as spin-coating polyoctylfluorene thin film before and after thermal annealing at 120oC.
The absorption peak at 380 nm and photoluminescence peaks at 422, 457 and 479 nm are in line with reference 5, which demonstrates that the as spin-coating polyoctylfluorene thin is amorphous.
In the normal X-ray diffraction pattern, only a sharp diffraction peak at 4.9 nm-1 corresponding to (200) of a phase polyoctylfluorene and a wide diffraction peak at 16.9 nm-1 corresponding to glass substrate can be observed.
References [1] Ron Mertens, The OLED Handbook: A Guide to OLED Technology, Industry & Market

Fig.1.
The band around 1385 cm-1 is belonging to the symmetrical deformation vibration of -CH3.
From the IR of MEG, it shows that the bands around 3701cm-1, 1739 cm-1 and 1280 cm-1are attributed to Mg (OH)2.
References [1] G.W.
Phys Stat Solidi (a), 1981, 65: 479-483

Ni-Mn-In Heusler alloy thin films grown by pulsed laser deposition Grunin A.1,*, Goikhman A.1, Rodionova V.1,2,3 1 Immanuel Kant Baltic Federal University, 236041 Kaliningrad, Russia 2 M.V.
Figure 1 shows the variation of In concentration within the films measured using AES.
References [1] L.
Sci.Forum 2243 (2004) 475–479
Hansen, Influence of growth temperature on phase and intermixing in Ni2MnIn Heusler films on InAs (0 0 1), J.

Figure 1.
References [1] K.
International Conference on Wireless Communication and Signal Processing (2009) 1-5
Zheng, Spectrum sensing algorithms for primary detection based on reliability in cognitive radio systems, Computers and Electrical Engineering, 36 (2010) 469-479
Secur. 1 (2009) 1-5

We defined our task as "Dangerous object capturing in surveillance web" as shown in Figure 1.
Figure 1.
Table.1 The experimental results of the proposed method.
Table 1 presents the performance in real surveillance applications.
Ponce, "HOT curves for modelling and recognition of smooth curved 3D objects," Image Vision Comput. 15, pp.479–498, 1997 [4] Peng Yao, Yongtian Wang, et.al, "Dangerous Object Recognition for Visual Surveillance", ICALIP, pp55-61, 2012 [5] C.

A schematic drawing of the compression test apparatus is shown in Figure 1[9].The sludge sample was inserted into the cylinder.
Basic properties of activated sludge such as solid content, organic material content, ash content,MLSS,SV30,SVI were showed in table 1.
Sep. 16 (1) (1979) 82–86
Technol. 28 (1) (1993) 189–192
-ASCE 123 (5) (1997) 479–485

These issues threaten the future development of human society and the health of Earth’s ecosystems [1].
Fig. 1 shows location and division of the seven regions.
The following Equations (refer with: Eq. 1) was used to extract NDVI values from the MOD13A3 data.
The result reflects the trend for the annual average NDVI during the study period [1].
[6] Ni J, Sykes MT, Prentice IC, Cramer W: Glob Ecol Biogeogr 9:463–479(2000)

Introduction The design of the new foundation structure of the rolling mill Block 1 in the Třinecké železárny is the subject of the article.
Developing of the Hydration Heat Recipe No. 1 is designed on a foundation slab (concrete C30/37; XC2; S4; Dmax22; 60-days).
References [1] Bažant, Z.P., Kim, J.
-E., Cohesive fracturing and stresses caused by hydration heat in massive concrete wall, Journal of Engineering Mechanics 129 (1), pp. 21-30, 2003
[9] Sun, W., Ni, F., Liu, L., Wu, Q., Zhao, R., Numerical analysis of hydration heat temperature characteristics of massive concrete, Jiangsu Daxue Xuebao (Ziran Kexue Ban)/Journal of Jiangsu University (Natural Science Edition)36 (4), pp. 475-479, 2014

The surface morphology of ion nitrocarburized layer is shown in Figure 1.
References [1] Cheng Zhao, Yu Wang.
Surface Technology, 2012, 41(1):83-85.
Heat Treatment of Metals, 2012, 37(1):68-71.
Surface Engineering, 2008, Key Engineering Materials Vols.373-374: 476-479