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SYNTHESIS AND CHARACTERIZATION OF L
- Page 3 and 4: STATEMENT BY AUTHOR This dissertati
- Page 5 and 6: Dedicated to ……… My beloved b
- Page 7 and 8: also thankful to all the members of
- Page 9 and 10: 2.3 Synthesis of binary oxide nanom
- Page 11 and 12: CHAPTER 5: Zinc Gallate ...........
- Page 13 and 14: imaging, scintillators, lasers, etc
- Page 15 and 16: morphology by heating at 500 and 90
- Page 17 and 18: nanoparticles having hexagonal stru
- Page 19 and 20: 100°C and 185°C, respectively in
- Page 21 and 22: into poly methyl methacryllate (PMM
- Page 23 and 24: 3. N. M. Dimitrijevic, Z. V. Saponj
- Page 25 and 26: Fig.13: Fig.14: (a) Simplified ray
- Page 27 and 28: Eu 3+ ions after heat treatment at
- Page 29 and 30: 615 nm Fig.50: FT-IR patterns (a) a
- Page 31 and 32: area electron diffraction pattern a
- Page 33 and 34: different amounts of Eu 3+ . Fig.86
- Page 35 and 36: and 545 nm, respectively. Fig.106:
- Page 37 and 38: List of Tables: Table 1: Variation
- Page 39 and 40: CHAPTER 1: Introduction 1.1 Histori
- Page 41 and 42: Rods, cylinders, wires and tubes ar
- Page 43 and 44: must be supersaturated either by di
- Page 45 and 46: - + - + charge stabilized nanoparti
- Page 47 and 48: exothermic reaction between the met
- Page 49 and 50: constant, ħ is h/2π, e is the ele
- Page 51 and 52: these platinum complexes have been
- Page 53: (IR), visible and ultra-violet (UV)
- Page 57 and 58: assisted by lattice phonons of appr
- Page 59 and 60: decay-time reduction is much easier
- Page 61 and 62: nanocrystals is shown in Fig.10 [58
- Page 63 and 64: depends strongly on the nature of t
- Page 65 and 66: corresponding emission and excitati
- Page 67 and 68: doped nanomaterials of the above me
- Page 69 and 70: will be formed and subsequently it
- Page 71 and 72: Eu 3+ ions were also subjected to s
- Page 73 and 74: transferred into a two-necked RB fl
- Page 75 and 76: Where λ is the wavelength of X-ray
- Page 77 and 78: Micro-structural characterization b
- Page 79 and 80: electrons (i.e. diffraction mode).
- Page 81 and 82: diffraction spots. By tilting a cry
- Page 83 and 84: surface. The contact mode can obtai
- Page 85 and 86: three types lines in the scattered
- Page 87 and 88: solids tend to be broadened because
- Page 89 and 90: sample fluoresce. The fluorescent l
- Page 91 and 92: pulse frequency) as excitation sour
- Page 93 and 94: Lanthanide ions doped Ga 2 O 3 nano
- Page 95 and 96: atoms at three corners and the lone
- Page 97 and 98: Figure 19 (a-d) shows SEM images of
- Page 99 and 100: Based on these results, it can be i
- Page 101 and 102: almost normal to the equatorial pla
- Page 103 and 104: Table 2. Summary of important modes
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systematic disappearance of these t
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comparison, Eu 3+ ions alone in wat
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the samples, suggesting that Eu 3+
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These inferences are further substa
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Similar DTA peaks have been reporte
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GaOOH samples doped with different
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The cell parameters increases with
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strong emission compared to corresp
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curves are shown in Fig.39. Lifetim
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Similar results are also observed f
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intensity of XRD peaks correspond t
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compared to the bulk material and a
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is almost 1½ times that of peak B1
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3.8 Interaction of Eu 3+ ions with
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The spectrum shows strong emission
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The decay curves are found to be bi
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As prepared undoped Sb 2 O 3 sample
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Intensity(arb.units) 1.0 0.8 0.6 0.
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3+ having surface lanthanide ions.
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diffraction patterns from the GaPO
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5 D 0 7 F 2 level to 7 F 7 7 1 , F
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The second possibility is the excha
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chemical shift anisotropy is much h
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not have strong interaction with th
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(001) (110) (011) (101) (020) (101)
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growth centre compared to higher vi
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observed after excitation at 250 an
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3+ 3+ concentration quenching. Tb l
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Compared to the selected area elect
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lattice. Lanthanide ions occupying
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obtained after 275 nm excitation is
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The luminescence dynamics associate
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that the broad peak can be resolved
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espectively. Value of this integral
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ethylene glycol moiety (stabilizing
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Room temperature and 100°C synthes
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heavier metal ion as compared to La
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Similar studies were also carried o
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3+ 3+ faster decay component is ass
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the other hand the Eu 3+ lifetime h
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3+ 4.4.8 Luminescence studies on Sm
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CHAPTER 5: Zinc gallate (ZnGa 2 O 4
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In pure EG an amorphous product is
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water content in the reaction mediu
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nucleation, thereby leading to incr
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particles. Thus the TEM studies als
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value. The lattice parameters calcu
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Quantum yield of the blue emission
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5.5.2. Eu 3+ doped ZnGa 1.5 In 0.5
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CHAPTER 6: Tungstates [MWO 4 (M = C
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ionic radius of the metal cation ca
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lattice. Asymmetric ratio is ~ 12 f
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700 Intensity (arb.units) 600 λ ex
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Intensity (arb.units) 25000 20000 1
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Strong green emission has been obse
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consists of strong band at 255 nm a
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peak can be attributed to the cryst
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nm) is observed from Er 3+ doped Ga
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and Dy 3+ doped CaWO 4 nanoparticle
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REFERENCES 1. D. J. Barber, I. C. F
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32. K. A. Gschneidner, Jr., L. Eyri
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65. Z. Deng, F. Tang, D. Chen, X. M
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100. A. Rouanel, J. J. Serra, K. Al
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130. F. Li, W. Jianhuai, L. Jiongti
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166. L. Fu, Z. Liu, Y. Liu, B. Han,
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205. R. Sasikala, V. Sudarsan, C. S
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238. E. Oldfield, R. A. Kinsey, K.
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271. B. G. Hyde, S. Andersson, ”I
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B. S. Naidu, B. Vishwanadh, V. Suda
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9. Room temperature synthesis of mu