Heiss W.D. (ed.) Quantum dots.. a doorway to - tiera.ru

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42 J.M. Elzerman et al. Vsource 250 Ω twisted pair powder filter computer computer fiber DAC 2 SGN SGN GND GND 100 µ V/ V 1 mV/ V 10 mV/ V 100 mV/ V connector box 0.22 nF OXFORD KELVINOX 300 0.4 nF 0.4 nF 0.5 nF 0.5 nF 0.5 nF 0.5 nF cold ground cold finger 0.4 nF 0.4 nF (20 nF) (20 nF) sample IVconverter ISOamp clean ground GND GND DMM x1 x10 4 GPIB SGN SGN 250 Ω twisted pair powder filter ELECTRONICS 10 MΩ 100 M 1G Ω Ω R FB SAMPLE ROOM-T BASE-T Fig. 11. Electrical circuit for performing a voltage-biased current measurement. Elements shown in gray are connected to ground. Gray lines indicate the shielding of the measurement electronics and wires
250 Ω twisted pair 20 MΩ powder filter Semiconductor Few-Electron Quantum Dots as Spin Qubits 43 SGN SGN GND GND fiber DAC 3 DAC 4 ....... DAC 8 connector box 0.22 nF OXFORD KELVINOX 300 clean ground 0.4 nF 0.4 nF 0.5 nF 0.5 nF 0.5 nF 0.5 nF cold ground 10 MΩ 10 MΩ cold finger 0.4 nF 0.4 nF (20 nF) (20 nF) 10 aF 10 aF sample GND GND SGN SGN 250 Ω twisted pair 20 MΩ powder filter ELECTRONICS SAMPLE ROOM-T BASE-T Fig. 12. Electrical circuit for applying voltages to the gate electrodes. Elements shown in gray are connected to ground. Gray lines indicate the shielding of the measurement electronics and wires
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 ...
Page 11 and 12: 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
Page 17 and 18: where � is a shorthand: � ≡ 3
Page 19 and 20: RG for Interacting Fermions 9 These
Page 21 and 22: RG for Interacting Fermions 11 is i
Page 23 and 24: RG for Interacting Fermions 13 the
Page 25 and 26: RG for Interacting Fermions 15 this
Page 27 and 28: RG for Interacting Fermions 17 equa
Page 29 and 30: � p � dθp = g 2π RG for Inter
Page 31 and 32: RG for Interacting Fermions 21 the
Page 33 and 34: References RG for Interacting Fermi
Page 35 and 36: Semiconductor Few-Electron Quantum
Page 39 and 40: 1.2 Implementations Semiconductor F
Page 43 and 44: GaAs n-AlGaAs AlGaAs GaAs Semicondu
Page 49 and 50: ε1 ε0 e Semiconductor Few-Electro
Page 51: 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 and 104:
Semiconductor Few-Electron Quantum
Page 105 and 106:
Semiconductor Few-Electron Quantum
Page 107 and 108:
98 M. Pustilnik and L.I. Glazman Co
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100 M. Pustilnik and L.I. Glazman F
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102 M. Pustilnik and L.I. Glazman (
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104 M. Pustilnik and L.I. Glazman A
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106 M. Pustilnik and L.I. Glazman t
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110 M. Pustilnik and L.I. Glazman
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112 M. Pustilnik and L.I. Glazman f
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114 M. Pustilnik and L.I. Glazman 5
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116 M. Pustilnik and L.I. Glazman U
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Page 129 and 130:
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122 M. Pustilnik and L.I. Glazman d
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124 M. Pustilnik and L.I. Glazman G
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126 M. Pustilnik and L.I. Glazman d
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Page 139 and 140:
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132 C.W.J. Beenakker e e N I N S Fi
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134 C.W.J. Beenakker 2 Andreev Refl
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136 C.W.J. Beenakker F E x 8d/hv ga
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138 C.W.J. Beenakker and we have de
Page 149 and 150:
140 C.W.J. Beenakker A stroboscopic
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142 C.W.J. Beenakker largely indepe
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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).
Page 169 and 170:
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
Page 179 and 180:
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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