Damage formation and annealing studies of low energy ion implants ...

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Page 1 and 2:
Damage formation and annealing stud
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3.2.2.6 Other models 40 3.2.3 Other
Page 5 and 6:
Chapter 7 Interaction between Xe, F
Page 7 and 8:
List of Figures Figure 1.1 a) Schem
Page 9 and 10:
Figure 4.13 Variation in the kinema
Page 11 and 12:
Figure 6.10 MEIS energy spectra for
Page 13 and 14:
Figure 7.8 Combined MEIS Xe depth p
Page 15 and 16:
Abbreviations and Symbols a/c amorp
Page 17 and 18:
Abstract The work described in this
Page 19 and 20:
Chapter 7 5 M. Werner, J.A. van den
Page 21 and 22:
terminal (Vg), current cannot flow
Page 23 and 24:
This is an approximate average leve
Page 25 and 26:
the active channel, adjacent to the
Page 27 and 28: To continue to improve devices ther
Page 29 and 30: produces a device quality regrown l
Page 31 and 32: technique of channelling Rutherford
Page 33 and 34: 22 J.S Williams. Solid Phase Recrys
Page 35 and 36: and the probability of scattering t
Page 37 and 38: importance for many atomic collisio
Page 39 and 40: M1, V0, E0 Figure 2.2 Elastic scatt
Page 41 and 42: 2.3.1 Models for inelastic energy l
Page 43 and 44: dE/dx (ev/Ang) 10 1 Inelastic Energ
Page 45 and 46: dE/dx (eV/Ang) 125 100 75 50 25 0 2
Page 47 and 48: Figure 2.5 Results of TRIM simulati
Page 49 and 50: Chapter 3 Damage and Annealing proc
Page 51 and 52: the Si/SiO2 interface, consuming th
Page 53 and 54: On the basis that by creating an in
Page 55 and 56: Figure 3.4 Structure of crystalline
Page 57 and 58: a Si atom will suffer little angula
Page 59 and 60: 3.2.2.5 Homogeneous model (Critical
Page 61 and 62: Sputtering and atomic mixing play a
Page 63 and 64: and is approximately 25 times faste
Page 65 and 66: elevant dopants later. For equal co
Page 67 and 68: nearest neighbour distance (52). By
Page 69 and 70: Category I defects are produced whe
Page 71 and 72: thermal annealing (600 - 700 °C an
Page 73 and 74: Figure 3.11 Relationship between im
Page 75 and 76: defect pairs due to Coulomb attract
Page 77: ⎛ 〈 C ⎞ ⎛ ⎞ I 〉 〈 C V
Page 81 and 82: 67 H. Bracht. Diffusion Mechanism a
Page 83 and 84: Hall effect measurements were carri
Page 85 and 86: energy than one scattered from an a
Page 87 and 88: epresents a small improvement over
Page 89 and 90: (dE/dx)out multiplied by the path l
Page 91 and 92: they are small compared to the diff
Page 93 and 94: ackscattering (27). This fact forms
Page 95 and 96: Figure 4.7 a) Plot of a Gaussian di
Page 97 and 98: similar to the width of the error f
Page 99 and 100: UP Ion Beam SPIN Rotation Sample Sc
Page 101 and 102: Kinematic factor (K) 1.0 0.8 0.6 0.
Page 103 and 104: Figure 4.14 Illustration of the dou
Page 105 and 106: 4.2.2.4 Interpretation of spectra A
Page 107 and 108: with are comparatively small, ~ 0.5
Page 109 and 110: Inelastic energy loss (eV/Ang) 32 2
Page 111 and 112: iterative procedure is carried out
Page 113 and 114: Yield (couts per 5µC) 300 250 200
Page 115 and 116: SIMS experiments were also carried
Page 117 and 118: MEIS, using the scattering conditio
Page 119 and 120: 4.5 Sample production Samples have
Page 121 and 122: an N2/O2 environment to maintain an
Page 123 and 124: 38 M. Anderle, M. Barozzi, M. Bersa
Page 125 and 126: damage evolution behaviour observed
Page 127 and 128: Yield (counts per 5 µC) 250 200 15
Page 129 and 130:
essentially a “zero dose” profi
Page 131 and 132:
no longer “visible” in MEIS has
Page 133 and 134:
yield (cts / 5µC) 500 400 300 200
Page 135 and 136:
5.4 Conclusion MEIS analysis with a
Page 137 and 138:
Chapter 6 Annealing studies 6.1 Int
Page 139 and 140:
6.2.2.2 Results and Discussion Figu
Page 141 and 142:
theory predictions and X-ray fluore
Page 143 and 144:
implantation conditions are those u
Page 145 and 146:
a) b) c) Yield (counts per 5 µC) Y
Page 147 and 148:
greater than MEIS. SIMS is not sens
Page 149 and 150:
attributed to the interference betw
Page 151 and 152:
The as-implanted sample, with a bro
Page 153 and 154:
a) b) Yield (counts per 5 µC) Yiel
Page 155 and 156:
interface, as evidenced by the high
Page 157 and 158:
duration, is observed. MEIS results
Page 159 and 160:
Yield (counts per 5µC) 500 400 300
Page 161 and 162:
ack edges of the Si peaks are very
Page 163 and 164:
underneath the SiO2 layer, iii) it
Page 165 and 166:
R s (Ω/sq) 950 900 850 800 750 60
Page 167 and 168:
As concentration (at/cm 3 ) 1E22 1E
Page 169 and 170:
R s (Ω/sq) 950 900 850 800 750 70
Page 171 and 172:
Following annealing it was observed
Page 173 and 174:
∆a/a (x 10 -3 ) 4,0 epi550 3,5 3,
Page 175 and 176:
Yield (counts per 5 uC) 350 300 250
Page 177 and 178:
(FWHM). Concomitantly, As in the re
Page 179 and 180:
Yield (counts per 5 µC) 450 400 35
Page 181 and 182:
The higher temperature anneals carr
Page 183 and 184:
ecomes steeper for the sample annea
Page 185 and 186:
Figure 6.28 Schematic illustrations
Page 187 and 188:
and the 2D picture in Figure 6.31b)
Page 189 and 190:
6.5 Conclusion In summary, in this
Page 191 and 192:
20 L. Capello, T. H. Metzger, M. We
Page 193 and 194:
egarding B profiles relevant to the
Page 195 and 196:
Yield (counts per 5 µC) 400 300 20
Page 197 and 198:
TRIM AU 0.04 0.03 0.02 0.01 TRIM si
Page 199 and 200:
a) F profile PAI 3 keV BF2 b) F pro
Page 201 and 202:
Yield (counts per 5 µC) 20 15 10 5
Page 203 and 204:
the corresponding PAI sample, yield
Page 205 and 206:
amorphous matrix, (16) i.e. local c
Page 207 and 208:
21 M. Anderle, M. Bersani, D. Giube
Page 209 and 210:
stopped at depths beyond the observ
Page 211:
the role of each individual element
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