shot noise in mesoscopic conductors - Low Temperature Laboratory

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110 Ya.M. Blanter, M. Bu( ttiker / Physics Reports 336 (2000) 1}166 Thus, the new feature due to charging e!ects is the multi-stability of the system in the range of voltages between < and
The noise power (201) is strongly voltage dependent via the quantities c , J, and . In particular, for
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Ya.M. Blanter, M. BuK ttiker / Phys
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8. Concluding remarks, future prosp
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text; they are usually extensions o
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such reviews are not readily availa
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Ya.M. Blanter, M. Bu( ttiker / Phys
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The above considerations are, of co
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and the initial state of our two-pa
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2.3.3. Multi-terminal case We consi
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Note that in the absence of time-de
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equilibrium and shot noise. For low
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and S" e A e< dE ¹(E )[1!¹
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arrier, situated in the region !w/2
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we include weak localization e!ects
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Page 59 and 60: Edge channels in the quantum Hall e
Page 61 and 62: Fig. 19. (a) Geometry of a ring thr
Page 63 and 64: a manifestation of interference e!e
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Page 69 and 70: Physically, this corresponds to ele
Page 73 and 74: Our starting point is Eq. (51), whi
Page 77 and 78: introducing the transmission coe$ci
Page 79 and 80: investigated experimentally. A self
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Page 87 and 88: the sample. These electrons are des
Page 93 and 94: with D ,¹ (2!¹ ). Performing t
Page 97 and 98: For completeness, we mention that i
Page 107 and 108: We note here, however, that there i
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Page 113 and 114: Fig. 32. Experimental results of Ku
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Page 119 and 120: 6.3. Interaction ewects Ya.M. Blant
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Page 125 and 126: non-thermalized electrons, the high
Page 129 and 130: Fig. 34. Geometry of the chaotic ca
Page 133 and 134: which describes strictly ballistic
Page 141 and 142: approximately e/C. Between the peak
Page 149 and 150: Boltzmann}Langevin approach (see Se
Page 151 and 152: thermal to shot noise. It is, howev
Page 153 and 154: Note added in proof Ya.M. Blanter,
Page 155 and 156: and Lee et al. [340] obtain in this
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