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Charge Transfer Dynamics in Quantum
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DECLARATION I, hereby declare that
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ACKNOWLEDGEMENTS It is my privilege
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1.3.5. Defect Mediated Relaxation 2
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2. 8. 4. White Light Generation- 45
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6.2. Experimental 6.2.1.Synthesis o
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devices based on QDs it has been sh
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Furthermore generation of pump (~40
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shell). This clearly indicated that
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12. V. I. Klimov, J. Phys. Chem. B,
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1.13 Reactant and Product Potential
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light. Inset: Kinetic traces monito
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6.5 Transient decay kinetics of gra
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at 670 nm after exciting at 400 nm
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ABBREVIATIONS BET BQ CB CCD CdS CdT
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1 Chapter 1
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3 size dependent optical properties
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5 1.2. Physics of Semiconductors 1.
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7 As seen from the schematic, poten
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9 Substituting this in Schrödinger
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11 ( r, r ) ( r ) ( r ) (1.13) e
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13 E E E 2 2 2 EX ne, le nh,
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15 spherical symmetry of field. The
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17 gE ( ) 2Em 2 3 3 (1.25) For a
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19 1.3.2. Electron-Hole energy tran
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21 Impact Ionization Figure 1.7. Sc
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23 understanding on mechanistic asp
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25 carriers are unable to sample th
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27 CB VB QD Metal Figure. 1. 10. Sc
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29 energy barrier. Therefore it is
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31 1 f q 2 A qB (1.30) 2 In equa
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33 Vibrational contribution can be
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35 1. 7. 1. Electron Injection ET i
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37 Under assumption of invariance o
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39 distribution. To achieve good si
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41 initially achieved monodispersit
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43 and rate of charge transfer acro
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45 1.32 P. V. Kamat, J. Phys. Chem.
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47 Chapter 2
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49 chemical species. Since a partic
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51 fluorescence forms an important
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53 eliminated by use of standard wh
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55 sample. Raman spectroscopy is ba
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57 will appear bright and region wi
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59 volatile solvent is drop casted
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61 spots arise from diffraction fro
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63 The electrical signal is then ch
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65 delayed and inverted. The two si
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67 Pump-probe technique is one of t
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69 Amplifier Jade Stretcher fs Osci
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71 Figure 2.6. Optical layout of Ti
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73 Grating Convex Mirror Concave Mi
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75 changes the polarization from ho
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77 Grating Output Input Mirror Grat
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79 μJ has a very high peak power.
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81 2.6. Dynamical Theory of X-Ray D
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83 Chapter 3
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85 Therefore the study of interfaci
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87 3. 2. Experimental Section 3.2.1
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89 and intensity show absence of ot
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91 which is also neutral; therefore
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93 electron transfer times. This re
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95 r B a * 0 3.1 me / me Now the
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97 nonadiabatic case the electron t
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99 drastically reduced leading to a
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101 While the study of injection dy
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103 study. Based on the injection d
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105 17. L. E. Brus, J. Phys. Chem.
- Page 151: 107 Chapter 4
- Page 154 and 155: 109 of the QDs. As a result surface
- Page 156 and 157: 111 4.2.2. Synthesis: The CdTe QDs
- Page 158 and 159: 113 lower hole state. In CdSe the l
- Page 160 and 161: 115 4.2 inset. The kinetic traces a
- Page 162 and 163: 117 growth of the bleach kinetics (
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- Page 170 and 171: 125 4.5. References 4.1. Efros, Al.
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- Page 176 and 177: 129 been made in the synthesis of t
- Page 178 and 179: 131 metallic synthesis by arrested
- Page 180 and 181: 133 5.3. Result and discussion: 5.3
- Page 182 and 183: 135 indicating a confinement induce
- Page 184 and 185: 137 absorption studies that on form
- Page 186 and 187: 139 1000 c b PL Intensity 100 10 a
- Page 188 and 189: 141 samples due to a very weak exci
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- Page 192 and 193: 145 Earlier authors [5.4] reported
- Page 194 and 195: 147 Sample t r(ps) t 1(ps) t 2(ps)
- Page 196 and 197: 149 In addition to the cooling dyna
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- Page 200 and 201: 153 5.20. Sreejith Kaniyankandy, Sa
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- Page 218 and 219: 170 as compared to that of GO. It i
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- Page 222 and 223: 174 A (m O.D.) 0 -10 -20 -30 a b Cd
- Page 224 and 225: 176 The cooling dynamics does not s
- Page 226 and 227: 178 The study clearly shows that th
- Page 228 and 229: 180 From emission studies both stea
- Page 230 and 231: 182 6.18. C. X. Guo, H. Bin Yang, Z
- Page 233 and 234: 184 CHAPTER 7 Summary and Outlook 7
- Page 235 and 236: 186 bleach growth times from 500fs
- Page 237 and 238: 188 Study of interfacial electron t
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