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APPENDIX A: LabVIEW PROGRAM <strong>FOR</strong> PEALD AUTOMATIC PROCESS 128
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CHEMICAL VAPOR DEPOSITION OF THIN F
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ABSTRACT Chemical vapor deposition
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DEDICATION This dissertation is ded
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φ In-plane tilt angle of X-ray dif
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ACKNOWLEDGMENTS It is my pleasure t
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CONTENTS ABSTRACT .................
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3.2.1 Introduction ................
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LIST OF TABLES Table 1. Hafnium ami
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indicated by the complex FMR curve.
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Fig. 49. Ferromagnetic resonance cu
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growth rate, good step coverage and
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growth of thin film oxides due to t
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one can uniformly deliver precursor
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for the next reaction step as shown
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Fig. 3. Schematic of a typical dire
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is predominantly dependent on syste
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J r J A -D n b-n 0 δ n or for the
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surface passivation with certain in
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ay spectroscopy (EDS), Wavelength d
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incidence angle is larger than cert
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epresenting those characteristic ph
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1.2.3.3 X-ray Diffraction (XRD) X-r
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exhibit diffraction peaks in the no
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(nanometers to tens of nanometers),
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strongest absorption of microwave s
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pinch-off to indicate the lack of a
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coupling is from unbound ferrite-fe
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diffusion barrier material in micro
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Fig. 14. A cross sectional scanning
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In spite of the same spinel structu
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ferrites has been investigated exte
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systems is showed in Fig.18.[83] As
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precursor vaporization process, e.g
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CHAPTER 3. PLASMA ENHANCED ATOMIC L
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the initial surface chemistry for t
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delay time of 2 seconds between spe
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Kcal/mol respectively. The stronger
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negative slope) behavior in the pum
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the existence of both physisorbed a
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decomposition products (Hf-H) and g
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dried by ultra high purity N2 gas.
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pressure for XPS analysis is around
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Hf and N elements, incorporation of
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[150,151] This is a unique feature
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software. The thickness results are
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CHAPTER 4. DIRECT LIQUID INJECTION
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film growth region. The properties
- Page 95 and 96: solution was accurately controlled
- Page 97 and 98: size). For the rocking curve analys
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- Page 103 and 104: Fig. 40. Cross-sectional view by fi
- Page 105 and 106: the MgAl2O4 substrate confirms cube
- Page 107 and 108: pattern. Fig.44(b) has diffraction
- Page 109 and 110: We have used an AGM (Alternating Gr
- Page 111 and 112: as derived equations for different
- Page 113 and 114: deposited at 600˚C is the lowest.
- Page 115 and 116: wave states degenerate with the FMR
- Page 117 and 118: Fig. 53. ϕ-scan of nickel ferrite
- Page 119 and 120: Surface roughness characterized by
- Page 121 and 122: Fig. 56. X-ray diffraction θ-2θ c
- Page 123 and 124: 4.4 Conclusion In summary, we have
- Page 125 and 126: CHAPTER 5. DIRECT LIQUID INJECTION
- Page 127 and 128: eaction zone of the tube furnace is
- Page 129 and 130: Fig. 58. X-ray diffraction characte
- Page 131 and 132: interface. This phenomenon probably
- Page 133 and 134: 6.1 Conclusion CHAPTER 6. CONCLUSIO
- Page 135 and 136: the temperature range of 600˚C to
- Page 137 and 138: such as PMN-PT and PZN-PT. CVD proc
- Page 139 and 140: [18]. L. S.-J. Peng, X. X. Xi, B. H
- Page 141 and 142: [54]. B. O. Johansson, J. -E. Sundg
- Page 143 and 144: [96]. J. D. Adam, S. V. Krishnaswam
- Page 145: [136]. J. Zhao, V. Fuflyigin, F. Wa
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