shot noise in mesoscopic conductors - Low Temperature Laboratory

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100 Ya.M. Blanter, M. Bu( ttiker / Physics Reports 336 (2000) 1}166 discussed by Aver<strong>in</strong> [205]. The probability of these transitions, which exist even at zero temperature, is "exp(!(1!¹)/e
Ya.M. Blanter, M. Bu( ttiker / Physics Reports 336 (2000) 1}166 101 Fig. 29. Experimental results of Dieleman et al. [211]. The Fano factor (plotted here as an e!ective charge, black squares) is compared with the theoretical prediction (solid l<strong>in</strong>e). Copyright 1997 by the American Physical Society. of the Fano factor (which is theoretically predicted to be 2/e< for e
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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
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Page 69 and 70: Physically, this corresponds to ele
Page 73 and 74: Our starting point is Eq. (51), whi
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Page 97 and 98: For completeness, we mention that i
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Page 107 and 108: We note here, however, that there i
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Page 129 and 130: Fig. 34. Geometry of the chaotic ca
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Page 149 and 150: Boltzmann}Langevin approach (see Se
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thermal to shot noise. It is, howev
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Note added in proof Ya.M. Blanter,
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and Lee et al. [340] obtain in this
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