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Additional 1 wt% Tm2O3 + 2 wt% Yb2O3 and 1 wt% Sm2O3 were introduced in heavy and light RE ions doped LYAS glasses based on the host weight, respectively.
Fig. 1 DTA curve of the 1 wt% Tm2O3 and 2 wt% Yb2O3 co-doped LYAS glasses.
Fig. 2 DTA curve of the 1 wt% Sm2O3 single-doped LYAS glasses.
Table 1 Characteristic temperatures of several optical glasses Composition Tg (°C) Tx (°C) Tc (°C) DT (°C) Ref.
Compd. 479 (2009) 883−887

Results Figure 1 shows the optical microstructures of the Al–oxide master alloy prepared.
(a) (b) Fig. 1.
The grain size further reached 370 µm at an addition of 1.7wt%.
References [1] D.G.
A, 361 (2003) 479-495 [11] G.I.

Along with this, passing chains of AAm and AA homo - and copolymers can be formed in the reaction mixture (Fig. 1).
Fig. 1.
In IR spectra of hydrogels washed from unreacted monomers and unbound homopolymers absorption bands corresponding to fluctuations of-C÷O, –C=O groups of AA (1452 cm-1, 1669 cm-1) are observed (Fig.2).
References [1] M.
Ferfera-Harrar, Synthesis and Properties of Chitosan-Graft Polyacry lamide/Gelatin Superabsorbent Composites for Wastewater Purification, Istanbul Turkey. 17 (2015) 479-503

Temperature dependence of photoluminescent spectra of samples A (ZnO nanorods with diameter of about 30 nm and length of about 300 nm) and B (ZnO nanorods with diameter of about 30 nm and small aspect ratios) can be seen in Fig. 1 a and 1 b, respectively.
As seen in curves 1) and 2) of Fig. 2 a, energies of exciton emissions for the samples A and B were plotted as a function of temperature.
References [1] Y.
Fan, The photoluminescence of ZnO thin films grown on Si (1 0 0) substrate by plasma-enhanced chemical vapor deposition, J.
Crystal Growth 240 (2002) 479-483

Strain rate used was 6.4×10-4 s-1.
It Fig. 1.
Summary 1.
References [1] C.D.
Forum Vol . 475-479 (2005), p. 457 [8] S.S.

Let the following be the parameters for the case: q=33.33, p=20US$/bbl, s=0.22p.a., r=0.1p.a., PM=45,l=0.15p.a., =20, T=5years, D=5.25US$/bbl, h =0.03 (US$/bbl)-1.year-1.
Figure 1.
Acknowledgements This work was financially supported by the national social science fund (12BJL074) , Social Science Project of Chinese Ministry of Education(Major Program), References [1] Dias, M., “Valuation of exploration and production assets: an overview of real options models,” Journal of Petroleum Science and Engineering, 2004. 44(1-2): pp. 93-114
[6] Paddock, J.L., Siegel, D.R., Smith, J.L., “Option valuation of claims on real assets: the case of offshore petroleum leases,” Quarterly Journal of Economics, August 1988, pp.479– 508
[7] Pindyck, R.S., “The long-run evolution of energy prices,” Energy Journal , 1999,20 (2):pp.1– 27

Results and Discussion Fig. 1 is the emission spectra of glasses doped with the active ions.
Table 1 shows fluorescence lifetimes of the active ions doped Ge25Ga5Sb5Se65 glasses.
The immediate stage where the donor-donor interaction becomes important, the decay follows an exponential behavior at a rate determined by the following equation: 1/τm = 1/τ0 + VCDyCTm (1) Where τm is measured lifetime, τ0 is the lifetime of Tm3+ single-doped sample, V is a constant related to transfer constants, CDy and CTm represent Dy 3+ and Tm3+ concentrations, respectively.
Table 1 Fluorescence lifetimes of active ions doped Ge25Ga5Sb5Se65 glasses Dopant Wavelength (µm) Lifetime (µs) 0.05at% Dy 3+ 1.34 310 0.05at% Tm3+ 1.22 676 0.05at% Dy 3++0.05at% Tm3+ 1.34 /1.22 344 / 479 0.05at% Dy 3++0.1at% Tm3+ 1.34 370 0.05at% Dy 3++0.15at% Tm3+ 1.34 429 0.05at% Dy 3++0.2at% Tm3+ 1.34 471 Fig.5 Fluorescence decay curve of the Tm3+: 3H5→ 3H6 transition for 0.05 at% Dy 3+ and 0.05 at% Tm3+ co-doped glass.
References [1] K.

Table 1 summurizes results for I-V curve in Fig. 4.
References [1] E.
[3] Jang YH, Xin X, Byun M et al, An unconventional route to high efficiency dye-sensitized solar cells via embedding graphitic thin films into TiO2 nanoparticles photoanode, Nano Lett 12 (2012) 479-485 [4] M.
Sci Technol. 2(1) (2012) 54-75 [11] U.
Journal of Nanomaterials, 2017 (2017) 1-13

Positron Spectroscopy of Defects in Hydrogen-Saturated Zirconium BORDULEV Yuriy S.1, a *, LEE K. 1, b, LAPTEV Roman S. 1, c, KUDIIAROV Viktor N. 1,d and LIDER Andrey M. 1, e 1 National Research Tomsk Polytechnic University, Russia, Tomsk, Lenin Avenue 30, 634050 abus@tpu.ru, blibeichen@hotmail.com.tw, claptevrs@tpu.ru, dkudiyarov@tpu.ru, elider@tpu.ru Keywords: zirconium-hydrogen, defects, hydrogen embrittlement, positron lifetime.
As it can be seen from the Fig. 1.
Results and Discussions The dependence of average positron lifetime on hydrogen concentration is shown in Fig. 1.
References [1] A.
Pundt, Journal of Alloys and Compounds. 446-447 (2007) 479-483

The results are presented by overset grids (Ref. [10]) and by Fluent6.1 (Ref. [11]).
(a) present work (b) by overset grids,Ref[9] (c) by Fluent6.1,Ref[10].)
The results of time-average thrust coefficient, input power coefficient and thrust propulsive efficiency are listed in Table 1.
References [1] Lai J C S, Platzer M F.
Flugwiss, 13: 472-479(1965)