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Optimization of deposition temperature of SILAR Cu-rich CuInS2 thin films

.1088/0268-1242/20/8/006 [20] Shi Y., Jin Z., Li C., An H., Qiu J., Appl. Surf. Sci., 252 (2006), 3737. http://dx.doi.org/10.1016/j.apsusc.2005.05.055 [21] Kelly C.V., Jin M.H.C., Banger K.K., Mcnatt J.S., Dickman J.E., Hepp A.F., Mater. Sci. Eng. B, 116 (2005), 403. http://dx.doi.org/10.1016/j.mseb.2004.09.033 [22] Dhanam M., Kavitha B., Velumani S., Mater. Sci. Eng. B, 174 (2010), 209. http://dx.doi.org/10.1016/j.mseb.2010.03.028 [23] Zeaiter K., Llinares Y., Llinares C., Sol. Energy Mater. Sol. Cells., 61 (2000

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Formation of Fe and Ni substituted LiMn2–XMXO4 nanopowders and their crystal and electronic structure and magnetic properties

temperature to 300 °C with the heating rate of 10 °C/min and maintained at this temperature for 3 hours. Then, the samples were heated at the same rate to 700 °C and maintained at this temperature for next 5 hours. After completion of the calcination stage the nanocrystalline powders were cooled down freely. For the iron doped series, the chelating agent: citric acid monohydrate (C 6 H 8 O 7 ·H 2 O) with ethylene glycol (99 % CHEMPUR) were added to the solution. The solutions were dried for several hours at 150 °C. The obtained powders were ground in an agate mortar and

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Carbonaceous materials for adsorptive refrigerators

M., Rodriguez L., De Lucas A., Rodriguez J.F., Int. J. Refri., 29 (2006), 30. http://dx.doi.org/10.1016/j.ijrefrig.2005.05.005 [14] Rouquerol J., Avnir D., Fairbridge C.W., Everett D.H., Haynes J.H., Pernicone N., Ramsay J.D.F., Sing K.S.W., Unger K.K., Pure Appl. Chem., 66 (1994), 1739. http://dx.doi.org/10.1351/pac199466081739 [15] Buczek B., Wolak E., Adsorption, 14 (2008), 283. http://dx.doi.org/10.1007/s10450-007-9094-5

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Complex permittivity, permeability and microwave absorbing properties of Co–Ti substituted strontium hexaferrite

M-type hexagonal ferrites with compositions SrFe (12-2x) Co x Ti x O 19 (x = 0.0, 0.3, 0.5, 0.7, 1.0), were synthesized by the conventional ceramic processing method. The detailed procedure of the synthesis has been published in our previous paper [8] . The pellets were sintered in air at a temperature of 1300 °C for 12 hours in an electric furnace. Then the pellets were shaped to fit exactly into a 10.16 × 22.86 mm 2 rectangular X-band waveguide (WR-90). The complex scattering parameters that correspond to the reflection (S 11 or S 22 ) and transmission (S 21

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Sol-gel-derived hybrid materials multi-doped with rare-earth metal ions

., Benalloul P., Stręk W., Anh T.K., Materials Science, 20 (2002), 47. [10] Yan B., Materials Letters, 57 (2003), 2535. http://dx.doi.org/10.1016/S0167-577X(02)01307-1 [11] Schraml-Marth M., Walther K.L., Wokaun A., Handy B.E., Baiker A., J. Non-Cryst. Solids, 143 (1992), 93. http://dx.doi.org/10.1016/S0022-3093(05)80557-5 [12] Song C.F., Lü M.K., Yang P., Xu D., Yuan D.R., Thin Solid Films, 413 (2002), 155. http://dx.doi.org/10.1016/S0040-6090(02)00440-6 [13] Fox A

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Optical and surface morphological studies on CuPcOC8 thin films prepared by physical vapour deposition

., Friedman B., Appl. Surf. Sci. 205 (2003), 274. http://dx.doi.org/10.1016/S0169-4332(02)01115-7 [39] Joseph B., Menon C.S., E-J. Chem., 5 (2008), 86. http://dx.doi.org/10.1155/2008/102948 [40] Pankove J.T., Optical Processes in Semiconductors, Prentice Hall, Inc. Englewood Cliffs, New Jersey, USA, (1970), 36. [41] Karan S., Mallik B., Solid State Communications, 143, (2007), 289. http://dx.doi.org/10.1016/j.ssc.2007.05.043

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Capacitive behavior of highly-oxidized graphite

[1] Brodie B.C., Philos. T. R. Soc. A, 149 (1859), 249. http://dx.doi.org/10.1098/rstl.1859.0013 [2] Staudenmaier L., Ber. Dtsch. Chem. Ges., 31 (1898), 1481. http://dx.doi.org/10.1002/cber.18980310237 [3] Hummers W.S., Offeman R.E., J. Am. Chem. Soc., 80 (1958), 1339. http://dx.doi.org/10.1021/ja01539a017 [4] Jeong H.-K., Lee Y.P., Lahaye R.J.W.E., Park M.-H., An K.H., Kim I.J., Yang C.-W., Park C.Y., Ruoff R.S., Lee Y.H., J. Am. Chem. Soc., 130 (2008), 1362

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FeS2 quantum dots sensitized nanostructured TiO2 solar cell: photoelectrochemical and photoinduced absorption spectroscopy studies

[1] O’Regan B., Grätzel M., Nature, 353, (1991), 737. http://dx.doi.org/10.1038/353737a0 [2] Bedja I., Hotchandani S., Kamat P.V., J. Phys. Chem., 98, (1994), 4133. http://dx.doi.org/10.1021/j100066a037 [3] Bedja I., Hotchandani S., Kamat J., Appl. Phys., 80, (1996), 8. [4] Heimer T.A., Heilweil E.J., Bignozzi C.A., Meyer, G.J., J. Phys.Chem. A, 104, (2000), 4256. http://dx.doi.org/10.1021/jp993438y [5] Liu D., Kamat P.V., J

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Some observations on the synthesis and electrolytic properties of (Ba1-xCax) (M0.9Y0.1)O3, M = Ce, Zr-based samples modified with calcium

compositions BaCe0.9Y0.1O3, (Ba 0.98 Ca 0.02 )(Ce 0.9 Y 0.1 )O 3 , (Ba 0.95 Ca 0.05 )(Ce 0.9 Y 0.1 )O 3 , and (Ba 0.90 Ca 0.1 ) (Ce 0.9 Y 0.1 )O 3 , designated subsequently as BCY, C2BCY, C5BCY, and C10BCY, respectively. A similar procedure was applied to a series of samples involving barium zirconate, such as: BaZr 0.9 Y 0.1 O 3 , (Ba 0.98 Ca 0.02 ) (Zr 0.9 Y 0.1 ) O 3 , (Ba 0.95 Ca 0.05 ) (Zr 0.9 Y 0.1 )O 3 and (Ba 0.9 Ca 0.1 ) (Zr 0.9 Y 0.1 )O 3 depicted in this paper as BZY, C2BZY, C5BZY and C10BZY. Studies on thermal decomposition processes of (Ba 1-x Ca x )(M 0.9 Y

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Electrospinning synthesis of 3D porous NiO nanorods as anode material for lithium-ion batteries

.H., J. Power Sources , 183 (2008), 717. 10.1016/j.jpowsour.2008.05.079 Wang L. Yu Y. Chen P.C. Zhang D.W. Chen C.H. J. Power Sources 183 2008 717 [10] Fan Q., Whittingham M.S., Electrochem. Solid. St ., 10 (2007), 48. 10.1149/1.2422749 Fan Q. Whittingham M.S. Electrochem. Solid. St 10 2007 48 [11] Ji L.W., Lin Z., Zhou R., Shi Q., Toprakci O., Medford A.J., Electrochim. Acta , 55 (2010), 1605. 10.1016/j.electacta.2009.10.033 Ji L.W. Lin Z. Zhou R. Shi Q. Toprakci O. Medford A.J. Electrochim. Acta 55 2010 1605 [12] Cui Q.Z., Dong X.T., Wang J.X., Li M

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