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Page 1 and 2:
Lecture Notes in Physics Editorial
Page 3 and 4:
W. Dieter Heiss (Ed.) Quantum Dots:
Page 5:
Preface Nanoscale physics, nowadays
Page 9 and 10:
Contents A Guide for the Reader ...
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A Guide for the Reader Quantum dots
Page 13 and 14:
The Renormalization Group Approach
Page 15 and 16:
RG for Interacting Fermions 5 where
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where � is a shorthand: � ≡ 3
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RG for Interacting Fermions 9 These
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RG for Interacting Fermions 11 is i
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RG for Interacting Fermions 13 the
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RG for Interacting Fermions 15 this
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RG for Interacting Fermions 17 equa
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� p � dθp = g 2π RG for Inter
Page 31 and 32:
RG for Interacting Fermions 21 the
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References RG for Interacting Fermi
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Semiconductor Few-Electron Quantum
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1.2 Implementations Semiconductor F
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GaAs n-AlGaAs AlGaAs GaAs Semicondu
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Page 47 and 48:
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ε1 ε0 e Semiconductor Few-Electro
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Page 53 and 54: 250 Ω twisted pair 20 MΩ powder
Page 55 and 56: Semiconductor Few-Electron Quantum
Page 61 and 62: 10 5 0 -5 Semiconductor Few-Electro
Page 63 and 64: G ( e / h) 2 2 1 0 Semiconductor Fe
Page 67 and 68: V R (V) V R (V) Semiconductor Few-E
Page 69 and 70: V L (V) -1.084 -1.082 -1.080 -1.078
Page 71 and 72: B // Semiconductor Few-Electron Qua
Page 77 and 78: a RESERVOIR 200 nm Semiconductor Fe
Page 81 and 82: 4.5 QPC Versus SET Semiconductor Fe
Page 83 and 84: a reservoir dot Semiconductor Few-E
Page 85 and 86: a b c V P (mV) 10 5 0 ∆I QPC E F
Page 91 and 92: Spin-down counts 200 100 a Semicond
Page 101 and 102: 6.7 Unresolved Issues Semiconductor
Page 103: Semiconductor Few-Electron Quantum
Page 107 and 108: 98 M. Pustilnik and L.I. Glazman Co
Page 109 and 110: 100 M. Pustilnik and L.I. Glazman F
Page 111 and 112: 102 M. Pustilnik and L.I. Glazman (
Page 113 and 114: 104 M. Pustilnik and L.I. Glazman A
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Page 125 and 126: 116 M. Pustilnik and L.I. Glazman U
Page 131 and 132: 122 M. Pustilnik and L.I. Glazman d
Page 133 and 134: 124 M. Pustilnik and L.I. Glazman G
Page 135 and 136: 126 M. Pustilnik and L.I. Glazman d
Page 141 and 142: 132 C.W.J. Beenakker e e N I N S Fi
Page 143 and 144: 134 C.W.J. Beenakker 2 Andreev Refl
Page 145 and 146: 136 C.W.J. Beenakker F E x 8d/hv ga
Page 147 and 148: 138 C.W.J. Beenakker and we have de
Page 149 and 150: 140 C.W.J. Beenakker A stroboscopic
Page 151 and 152: 142 C.W.J. Beenakker largely indepe
Page 153 and 154: 144 C.W.J. Beenakker The effective
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146 C.W.J. Beenakker Fig. 6. Ensemb
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148 C.W.J. Beenakker 1.4 1.2 1.0 0.
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150 C.W.J. Beenakker 〈ρ(E)〉 =
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152 C.W.J. Beenakker P 0.5 0.4 0.3
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154 C.W.J. Beenakker P(x) 0.4 0.3 0
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156 C.W.J. Beenakker tunnel/ Egap 4
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158 C.W.J. Beenakker its momentum).
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160 C.W.J. Beenakker E00 = π� =
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162 C.W.J. Beenakker 〈ρ(E)〉 δ
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164 C.W.J. Beenakker As described i
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166 C.W.J. Beenakker 0.30 � Egap
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168 C.W.J. Beenakker The τE-depend
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170 C.W.J. Beenakker that a fully m
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172 C.W.J. Beenakker (τ−,τ+), w
Page 183:
174 C.W.J. Beenakker 61. P. G. Silv
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