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17 N
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29 r = 0.88
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43 P x λ P x λ
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45 d m = d 1/ m, d m i 1...m ( d i ) 2 = c c i m
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53 d
54 β = 1 β = 1.5 β = 2 β = 3 d b = d a d b = 1.0 d b = 2.0 d b = 3.0 β = 1 β = 2 β = 3 d a d a χ 2 β d b
55 m m
56
57
58 µ A d A,B d A µ N µ B d B µ N A B µ N µ A d A A B A B d A,B A B d, = 2d, d d d d,
59 2 2 d d = 2z [P (C)], z [ ] z P(C) ϕ A (c) ϕ B (c) = 1, c ϕ A B
60 χ 2 χ 2 χ 2 χ 2 k k χ 2 χ 2 χ 2 χ 2 (d ) 2 d
61 µ C δ S µ C µ C + δ S c c + µ C δ S c c + µ C χ 2 HR c d ( HR = 1 F c; 1, (d ) 2), χ 2 FA FA = 1 F (c; 1), χ 2 c
62
63
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66 β = SE = p < 0.001
67
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69 β = SE = p = β = SE = p = d d
70 d d 1 m (d m) 2 = d m = d 1/ m + 1 d m = d 1/ m + c
71 d d d d a d m, = a d 1,, m d m, = a d m,.
72 d d d d d χ 2 = i C N i j R (p ij π ij ) 2 π ij, i j R C N i p ij π ij
73 d χ = G 2 + k (N), G 2 G 2 = 2 i C N i j R p ij (p ij /π ij ) k N i i N χ 2 G 2 d χ 2
74
75
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78 Px (C) P D (C) P D (C) P x(c) d χ 2 d d
79 d d d d d d d
80
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82 β = SE = p < β = SE = p = β = SE = p = 0.450
83
84
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86 m
87
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90 d χ d χ d χ d χ
91 d χ
92 χ 2 d d β β χ d d β β χ
93
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100 β = SE = p < β = SE = p < β = SE = p = 0.076
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102 A B p A p B p R p R = p A p B, t f(t) g(t) F (f) F (g) (f g) F 1 [F (f) F (g)], F 1 f g t
103
104 G 2 G 2 = 2 i N ij p ijk p ijk, π ijk j i j k N ij p ijk π ijk BIC = G 2 + k (N) k N G 2 G 2 k
105 G 2 G 2 G 2 G
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113 z s T T N (ν, η) a t ν η a T s T
114 d ν η σ
115 A B a T T er s T ν
116 G 2 0.1
117 ν α T α α α u m P(u m ) = ( ) i α m i<m ( m 1 i ) p i (1 p) m i 1, p p 1 2 m d m = d 1 m ν m
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119 ν η a T s T α T α ν α ν m = ν 1 m.
120 s t η t T
121 G 2 T ν t T T a t T a t T α t T T T T T
122 T T
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125 β = SE = p < β = SE = p < 0.001
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127 G 2 G 2 G 2 G β = SE = p < G 2
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129 G 2
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135 ν d a t T t ν d T t α t ν d a t T t α t ν ν t ν T
136 G 2 ν d a t T t ν d a t T t α t ν d a t T t α t ν d T t ν d a t T t a α ν d a t T t ν d T t α t ν α
137 ν d a t T t α t ν d a t T t ν d T t α t ν d a t T t α t
138 ν d a t T t
139 ν d T t α t α
140 ν d a t T t α t
141 ν α α
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149 T T ν d T t α t ν d a t T t ν d a t T t α t
150 G 2 T ν t T T T α t a t T G 2 T a t T T α t ν t T ν t a t T G 2 ν t T α t ν t a t T ν t T α t Tα t ν t a t T α t Tα t ν t a t T α t
151 G 2 T ν t T T α t a t T T G 2 a t T a t T α t ν t a t T a t T α t Tα t ν t a t α t
152 T ν sν a T st α Tα να T
153 T ν sν a T st α Tα να T
154 G 2 ν d T t α t ν d T t α t ν d T t α t ν d α ν T α t Tα t ν d T t α t ν d α G 2 ν T ν T ν d T t α t Tα ν t d α ν d T t α t Tα ν t d α ν d T t G 2 ν d a t T t ν d a t T t ν d a t T t α t ν d a t T t α t ν d a t T t α t ν d α
155 G 2 ν a t T α t Tα t ν a t T α t ν a t T α t Tα ν t t α ν a t T α t t ν a t T α t Tα ν t t α G 2 ν d T t ν d T t α t ν d T t α t ν T ν d T t
156 ν d T t α t ν sν a T st α Tα να ν d T t α t
157 ν d a t T t ν sν a T st α Tα να ν d a t T t
158 ν d a t T t α t ν sν a T st α Tα να ν d a t T t α t
159
160
161
162
163 π/4
164 3π/4
165 3π/4 π/4 π/4 3π/4 β = SE = p = β = SE = p < β = SE = p < 0.001
166
167
168 (d i,m) 2 = (1 f (b (θ i a))) (d 1 )2, m i m d 1 f ( ) a b d (d ) 2 d i,m = (1 f (b (θ i a))) d 1. m
169 , d (d ) 2 (d ) 2
170 θ P θ P θ P θ P (d ) 2 λ M λ M λ M / λ M = λ M f (θ) f : ( π, π) [0, 1] d = f (θ) λ M θ (0, f (θ))
171 θ 0 θ 0 π/2
172 (1 f ( )) f
173 m (d m) 2 =
174 G G 2 = 2 i A N i,j j B k R p i,j,k p i,j,k π i,j,k, i A j B k R N i,j p i,j,k π i,j,k < i, j, k >
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179 β = SE = p = β = SE = p = β = SE = p = 0.170
180 β = SE = p = β = SE = p = β = SE = p < β = SE = p < 0.001
181 d i,m = f (b (θi a)) d 1 ατ, m i m α τ
182 d i,m = f (b (θ i a)) d 1 ατ. m
183 m (d m) 2 = const
184 G
185 d
186
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190 G G G
191 G G
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195 G G G
196 G G
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200 β = SE = p < β = SE = p < β = SE = p < 0.001
201
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203 d (d i,m )2 m i (d i,m) 2 = (1 ϕ (bθ i)) (d 1 )2, m θ i i ϕ b d 1 ν ν i,m = (1 ϕ (bθi )) ν 1 m.
204 T l l T
205 η η G 2
206 T η α ν T l T s η s α s ν α ν α ν
207 G 2 η s T s ν α η s T s ν α T s ν α T s ν α η s T l ν α η s T s ν α
208 η s T s ν α η s T s ν α
209 η s T s ν α
210 T s ν α
211 T s ν α η s T s ν α
212 β = SE = p = 0.014
213 ν i,m = (1 ϕ (bθi )) ν 1 γτ m i m γ ϕ τ ν α
214
215 ν α ν α ν α ν α ν α ν l α ν t α ν α G 2 η s T s ν α η s T s ν α η s T s ν α η s T s ν t α η s T l ν α
216 ν s T s ν α γ
217 ν s T s ν α
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220 d 1 / m d 1 m η
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223 η s T s ν α ν s T s ν α
224 G 2 T s ν α T s ν α T s ν α η s T s ν α η s T s ν α G 2 T l ν α T l ν α T s ν α T s ν α η s T l ν α G 2 η s T s ν α T s ν α T s ν α T s ν α η s T s ν α
225 G 2 η s T s ν α η s T s ν α η s T s ν α η s T l ν α η s T l ν α G 2 η s T s ν α η s T l ν α η s T s ν α η s T s ν α η s T l ν α
226 η s T s ν α ν b η a T st α Tα να
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230 G 2 η s T s ν α η s T s ν α η s T s ν α η s T s ν α η s T s ν α G 2 η s T s ν α η s T l ν α η s T s ν l α η s T s ν α η s T l ν α G 2 η s T s ν α η s T s ν t α η s T s ν α η s T s ν α η s T s ν α
231 G 2 η s T s ν α η s T l ν α η s T l ν α η s T s ν α η s T l ν α G 2 η s T s ν α η s T s ν α η s T s ν α T s ν α T s ν α
232 η s T s ν α ν b γ η a T st α Tα να
233 N
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259 d M
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273 Minerva Access is the Institutional Repository of The University of Melbourne Author/s: Lilburn, Simon David Title: Information limits within visual short-term memory Date: 2016 Persistent Link: File Description: Information limits within visual short-term memory Terms and Conditions: Terms and Conditions: Copyright in works deposited in Minerva Access is retained by the copyright owner. The work may not be altered without permission from the copyright owner. Readers may only download, print and save electronic copies of whole works for their own personal non-commercial use. Any use that exceeds these limits requires permission from the copyright owner. Attribution is essential when quoting or paraphrasing from these works.
Chapter 10: BIM for Facilitation of Land Administration Systems in Australia
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May 3, 2012: Some news: luminous ultraviolet-optical flare from the nuclear region of an inactive galaxy at a redshift of on March 28, 2011,
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