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The glass transition temperatures of the HPAEK-F and HPAEK-OH are 114°C and 162°C respectively.
      
It was found by DSC measurements that the melting point of samples gradually shifted to lower temperatures with the decrease of the solution concentration used for sample preparation.
      
Polycrystal Li2B4O7 (LBO) doped with Cu and In was prepared and then sintered at different temperatures.
      
This scheme is a supplement to the conventional thermal decomposition of organometallic compounds at higher temperatures.
      
The swelling ratios of the hydrogels at different temperatures were measured.
      
Volumetric properties of glucose in aqueous HCl solutions at temperatures from 278.15 to 318.15 K
      
Results showed that the doped element of Cl lowered the temperatures of phase transformation of TiO2 from amorphous to anatase and from anatase to rutile.
      
Controlled/living photopolymerization of methyl methacrylate (MMA) in miniemulsion mediated by 4-hydroxy-2,2,6,6-tetramethyl-piperidinyloxy (HTEMPO) was carried out at ambient temperatures.
      
The results indicate that moisture moved in wood from the warm surface to the cold one even if opposite faces of the sealed wood assembly were exposed continuously to different but constant temperatures for a short period.
      
Compared with untreated wood and the PF-impreg, the pyrolysis process of WMNC changed; its starting decomposing temperature decreased and its pyrolysis weight loss at high temperatures greatly decreased.
      
This area has a harsh climate due to low temperatures and low air pressure at high elevations.
      
The equilibrium adsorption isotherms are calculated at five different temperatures ranging from 314 K to 376 K and compared with the experimental equilibrium adsorption isotherms.
      
At sufficiently low temperatures, the configurational phase space of a large spin-glass system breaks into many separated domains, each of which is referred to as a macroscopic state.
      
Size dependence of phase transition temperatures of ferromagnetic, ferroelectric and superconductive nanocrystals
      
The study showed that the longitudinal and transversal temperatures of output cold CH3CN beam could be about ~2 K and ~ 420 mK, and the corresponding guiding efficiency was about 10-5 as the guiding voltage was 3 kV.
      
Vegetative growth and asexual reproduction are especially vigorous during summer due to high temperatures and soil drought stress.
      
It was also determined that the best degradation temperatures were 37°C and pH 7.0 respectively.
      
The result indicated that the addition of nano-CaCO3 markedly increased the crystallization temperatures of PP and induced the formation of the β-crystal of PP.
      
The crystallization temperatures of nano-CaCO3/PP composites modified by reactive monomers were further increased, but the melting-peak intensity of the β-crystal of PP was not greatly influenced.
      
With the increase of crystallization temperatures, the double melting-peak moved toward the high-temperature side.
      
 

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