CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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61 spots arise from diffraction from a particular plane of a crystallite. The radial distance from the centre is related to the lattice spacing and TEM parameters. Since the magnification parameters of TEM are known, lattice spacing can be obtained. Now in a polycrystalline sample azimuthal orientation of crystals with respect to the optic axis is random. Therefore each of these crystals will diffract at different azimuthal angle creating a series of spots radially arranged around an axis as a result it appears like a ring. The position of the rings from the central maxima helps in phase characterization of a material. 2. 6. 3. Electron Energy Loss Spectroscopy (EELS) In a TEM the electrons impinging on sample are monoenergetic. On interaction with the sample electrons can undergo inelastic scattering. The loss of energy can correspond to plasmon and phonon excitation, band related transition, ionizations etc. These energy loss phenomena mentioned are very specific to a crystal. Additionally inner shell ionizations are specific to a particular element. Therefore we can obtain information on both elemental composition and crystalline property at the same time. This is accomplished by quantifying energy lost by electrons. Very often EELS is used to obtain elemental mapping in a particular sample [2.12]. 2.7. Time Correlated Single Photon Counting 2.7.1. Introduction Previous section dealt with steady state measurement i.e. measurement carried out under equilibrium. One can gain a greater insight into a system from measurements carried
62 out in time domain. For example in a biological system same fluorophore can have vastly different lifetimes depending upon environment. Such species can be easily monitored by a time domain measurements due to large spectral overlap between absorption and emission. Most commonly used time domain measurement is time correlated single photon countung. Here decay profile of a fluorophore is recorded after excitation. Modern TCSPC instruments use pulses as short as picoseconds by modelocking in conjunction with fast detectors, micro channel plate (MCP) and photomultiplier tube (PMT). However, commonly used TCSPC systems use LEDs as the light source and with PMT as detector. 2.7.2. Instrumentation A typical schematic is of working principle is given in figure 2.3. Principle of TCSPC is based on detection of delay time between excitation and emission photons [2.4, 2.13]. This is done under conditions where detection rate is less than 1 emission photon for 100 excitations. Therefore profile obtained under such conditions represents decay profile of a fluorophore. As shown in the schematic the start of the experiment is by detection of photons from light source which could be LED, laser or lamp etc depending on the instrument. Light source is divided into two parts. One part is sent to a photodiode producing an electrical signal which is sent to constant fraction discriminator (CFD). CFD defines exact point for the START for time to amplitude converter (TAC). TAC consists of the capacitor which charges when START signal arrives and stops when STOP signal arrives from the other CFD. The electrical output generated is proportional to time and forms the basis for time delay detection between START and STOP pulse. The other part excites the sample and emission is monochromatised by a monochromator and sent to PMT which detects emission photon.
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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
Page 52 and 53: 13 E E E 2 2 2 EX ne, le nh,
Page 54 and 55: 15 spherical symmetry of field. The
Page 56 and 57: 17 gE ( ) 2Em 2 3 3 (1.25) For a
Page 58 and 59: 19 1.3.2. Electron-Hole energy tran
Page 60 and 61: 21 Impact Ionization Figure 1.7. Sc
Page 62 and 63: 23 understanding on mechanistic asp
Page 64 and 65: 25 carriers are unable to sample th
Page 66 and 67: 27 CB VB QD Metal Figure. 1. 10. Sc
Page 68 and 69: 29 energy barrier. Therefore it is
Page 70 and 71: 31 1 f q 2 A qB (1.30) 2 In equa
Page 72 and 73: 33 Vibrational contribution can be
Page 74 and 75: 35 1. 7. 1. Electron Injection ET i
Page 76 and 77: 37 Under assumption of invariance o
Page 78 and 79: 39 distribution. To achieve good si
Page 80 and 81: 41 initially achieved monodispersit
Page 82 and 83: 43 and rate of charge transfer acro
Page 84 and 85: 45 1.32 P. V. Kamat, J. Phys. Chem.
Page 87: 47 Chapter 2
Page 90 and 91: 49 chemical species. Since a partic
Page 92 and 93: 51 fluorescence forms an important
Page 94 and 95: 53 eliminated by use of standard wh
Page 96 and 97: 55 sample. Raman spectroscopy is ba
Page 98 and 99: 57 will appear bright and region wi
Page 100 and 101: 59 volatile solvent is drop casted
Page 104 and 105: 63 The electrical signal is then ch
Page 106 and 107: 65 delayed and inverted. The two si
Page 108 and 109: 67 Pump-probe technique is one of t
Page 110 and 111: 69 Amplifier Jade Stretcher fs Osci
Page 112 and 113: 71 Figure 2.6. Optical layout of Ti
Page 114 and 115: 73 Grating Convex Mirror Concave Mi
Page 116 and 117: 75 changes the polarization from ho
Page 118 and 119: 77 Grating Output Input Mirror Grat
Page 120 and 121: 79 μJ has a very high peak power.
Page 122 and 123: 81 2.6. Dynamical Theory of X-Ray D
Page 128 and 129: 85 Therefore the study of interfaci
Page 130 and 131: 87 3. 2. Experimental Section 3.2.1
Page 132 and 133: 89 and intensity show absence of ot
Page 134 and 135: 91 which is also neutral; therefore
Page 136 and 137: 93 electron transfer times. This re
Page 138 and 139: 95 r B a * 0 3.1 me / me Now the
Page 140 and 141: 97 nonadiabatic case the electron t
Page 142 and 143: 99 drastically reduced leading to a
Page 144 and 145: 101 While the study of injection dy
Page 146 and 147: 103 study. Based on the injection d
Page 148 and 149: 105 17. L. E. Brus, J. Phys. Chem.
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109 of the QDs. As a result surface
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111 4.2.2. Synthesis: The CdTe QDs
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113 lower hole state. In CdSe the l
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115 4.2 inset. The kinetic traces a
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117 growth of the bleach kinetics (
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119 previous section we have discus
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121 lived charge transfer complex w
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123 100 times concentration of the
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125 4.5. References 4.1. Efros, Al.
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127 Chapter 5
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129 been made in the synthesis of t
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131 metallic synthesis by arrested
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133 5.3. Result and discussion: 5.3
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135 indicating a confinement induce
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137 absorption studies that on form
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139 1000 c b PL Intensity 100 10 a
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141 samples due to a very weak exci
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143 dynamical spectrum is negligibl
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145 Earlier authors [5.4] reported
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147 Sample t r(ps) t 1(ps) t 2(ps)
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149 In addition to the cooling dyna
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151 pulse-width time scale followed
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153 5.20. Sreejith Kaniyankandy, Sa
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155 CHAPTER 6 Charge Separation in
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157 Studies by Wang et. al. [6.15]
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159 graphene in a 1M NaOH solution.
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161 Intensity (a.u.) 5 4 3 2 1 CdTe
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163 dynamics of graphene oxide and
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165 GO as shown in the Figure 3 rev
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167 electron acceptor for Graphene.
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169 governs the recombination dynam
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171 Sample τ 1 (ps) τ 2 (ps) τ 3
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173 A (mO.D) 10.0 0.0 -10.0 -20.0 0
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175 involved in the relaxation may
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177 Electron quencher (benzoquinone
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179 Scheme 6.1. Schematic of Electr
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181 6.6. Reina, A.; Jia, X.; Ho, J.
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183 6.26. Kaiser, A. B.; Navarro, C
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185 assigned to injection into diff
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187 transfer from CdSe core to ZnTe
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189 However the position of bands i
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