- Page 1 and 2: SHG SPECTROSCOPY OF GALLIUM NITRIDE
- Page 3 and 4: COPYRIGHT vVilliam E. Angerer 1998
- Page 5 and 6: ACKNOWLEDGEMENTS I am most grateful
- Page 7 and 8: vi and support over the last three
- Page 9 and 10: viii and we report on photoluminesc
- Page 11 and 12: x 2.5 ~ovel Technique and Apparatus
- Page 13 and 14: Xll 7.3 7.2.3 Registering and Posit
- Page 15 and 16: xiv
- Page 17 and 18: xvi 2.10 Device for measuring ultra
- Page 19 and 20: xviii 6.5 Polarization and propagat
- Page 21 and 22: 2 scopies as a probe of these featu
- Page 23 and 24: 4 tionallinear microscopy is unable
- Page 25 and 26: 6 interference by group velocity mi
- Page 27 and 28: Chapter 2 Introduction to Nonlinear
- Page 29: 10 the electric fields as In this t
- Page 33 and 34: 14 2.3 (2) Xijk and Symmetry In gen
- Page 35 and 36: 16 X (2) zxx = ,\.zyy v(2) (2) = v(
- Page 37 and 38: 18 X~}k(W = 2wo) of our GaN samples
- Page 39 and 40: 20 nonlinear element of quartz, X~~
- Page 41 and 42: 22 the transmitted wave, E:t'°, Th
- Page 43 and 44: 24 150 I I "1 I :) ~ >- -. iii c v
- Page 45 and 46: 26 Quartz fundamental Figure 2.5: I
- Page 47 and 48: 28 The bound wave, which propagates
- Page 49 and 50: 30 1/e 2 its ma.'{imum value. This
- Page 51 and 52: 32 Here, x~;!Aw = 2wo) is a constan
- Page 53 and 54: 34 simplifications (2.39) and (2.40
- Page 55 and 56: 36 nonlinear waves. This model assu
- Page 57 and 58: 38 Fourier transform to E /2 (r, w)
- Page 59 and 60: 40 3 mm and with the parameters dis
- Page 61 and 62: 42 I " i iii iii iii iii iii iii ii
- Page 63 and 64: 44 parameter value Bl 2.35728 B2 -0
- Page 65 and 66: 46 is measured as a function of tra
- Page 67 and 68: 48 send pulse into device \11 input
- Page 69 and 70: 50 2.6 Conclusion In this brief sec
- Page 71 and 72: 52 LOCK-IN AMPLIAER LOCK-IN AMPLIAE
- Page 73 and 74: 54 After polarization, the beam was
- Page 75 and 76: 56 PO HR !l o IV team BP Figure 3.3
- Page 77 and 78: 58 .. ........... • / ~ '" ~ r --
- Page 79 and 80: 60 The production of ultrafast, hig
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62 800 ~ 0 0 J 0 0 0 0 J ~ 0 600~ 0
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64 measurements. Typically, I incre
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66 described below. Note that laser
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68 sentiallya nonlinear optical int
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70 780 800 820 840 860 880 900 920
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72 Unlike the linear spectroscopic
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74 fore, the ratio of these two qua
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76 of :UN is deposited on the Ah03
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78 computer HeNe Las polarizer chop
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80 ~------".... GaN A12a3 index flu
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82 + d I , GaN A12a3 Figure 4.3: Co
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84 4.2 Measurement of Indices of Re
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86 fields at the lh interface to th
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88 traveling wave, i.e. (-1.7) wher
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90 Note that the additional subscri
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92 £b, are defined only at the int
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94 Equations (4.30) and (4.32) are
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96 the calculation of the transmitt
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98 '- -0 OJ N 0.4 o E ~ o Z 0.2 o 2
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100 2.0 "'"" "I 1.5 E ::t ~ --c 0 -
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102 4.3 Photoluminescence of GaN To
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104 a photoluminescence measurement
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106 :J 0.01 0 ~ L ~ 0.008 r- :n :v
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108 0.08 ~. j -i ,-... I I ""I :::l
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Chapter 5 Properties of GaN In rece
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112 5.1 Crystal Structure :\ crucia
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114 PJO'tI [{fall Figure 5.1: \Vurz
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116 e 4 r .1 It Figure 5.2: Calcula
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118 Parameter Symbol Value electron
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120 high intrinsic electron concent
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122 equation (5.2), is represented
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124 C6v E E £l. 2C3 2C 3 2C6 2C 6
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126 gap, the nonlinear susceptibili
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128 rrb 10.0 eV -------- 5 9.0 eV r
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130 In> 1m> 1m>
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132 Emission of a photon on the bra
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134 5.5 MOCVD Growth of GaN Our GaN
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136 # dopant thickness mobility car
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138 6.1 Nonlinear Optical Spectrosc
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140 y lab X)lSlaJ / 2m Figure 6.1:
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142 Fig. 6.2 displays the azimuthal
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144 includes the effects of pulse p
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146 6.3 Theory of Nonlinear Optical
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148 L x i d 1 E( 00) air GaN sapphi
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150 wavevector components. The free
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152 z y x E( ro) air GaN Figure 6.5
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154 various free waves and summing
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156 factors are: the nonlinearity o
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158 where v /2 is the group velocit
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160 i N -' '- 0 ::J a 0 o.sf fiftH!
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162 4 ""' ::J en Q) - -' .D 2L ·oJ
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164 approximation. The agreement be
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166 midgap state) could playa role
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168 r: b S ~ r b I rs ~ r b I 0)1 r
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170 in various bonding geometries w
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, 172 .----. ::l U'J Q) ttl 0 '-.,;
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Chapter 7 SHG Microscopy The majori
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176 7.1 Historical Context of Secon
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178 comPJter - - - - - - - - - ~ ,-
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180 second-harmonic light towards t
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182 ~ 20 _____ ~ ____ J -----f- ---
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184 wave at normal incidence is (7.
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186 polarization is negligible for
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chopper AGate B Gate Signal Figure
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190 E 4000 1 c: 0 3000 ~ rJl -' 0 c
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192 depend on two components: a hig
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194 nanorope ~ Figure 7.8: Carbon n
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196 of light reflected from the sam
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198 mean square deviation, of the p
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200 7.3 Calculated SHG Signal from
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202 parameter symbol value laser re
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204 parameter symbol value surface
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Chapter 8 Conclusion In this brief
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208 properties of carbon nanotubes.
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210 that propagate through quartz a
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Appendix B Theory of Nonlinear Resp
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214 Fourier transforming equation (
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216 and (CA) with f.b == t(.:.vo) a
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218 The polarization, et, of the po
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220 and (0.1.,1) respectively. Equa
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Appendix E Effect of Sapphire Miscu
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224 with cosO 0 - sin (} o 1 o (E.3
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226 Let us compare the light transm
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228 , .............................
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230 it ( (fp·top..,(arr (ll, M r "
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232 nal-2.00 tab'(:r[ihi]-:r[ila] )
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234 1 - 2500.0; III - xU]; 1/ ti. t
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Bibliography [1] R. K. Chang~ J. Du
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238 [12] J. QL "V. Angerer, M. S. Y
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240 Diamond, SiC and Wide Bandgap S
- Page 261 and 262:
242 [40] M. M. Choy and R. L. Byer,
- Page 263 and 264:
244 [55] \V. P. Lin, P. M. Lundquis
- Page 265 and 266:
246 [70] J. vV. Yang, J. N. Kunzia,
- Page 267 and 268:
248 [85] B. Monemar and O. Lagerste
- Page 269 and 270:
250 [99] R. C. Miller, Optical Seco
- Page 271 and 272:
252 [114] "V. de HeeL W. S. Bacsa,