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- Page 3 and 4: 8. Concluding remarks, future prosp
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- Page 7 and 8: such reviews are not readily availa
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- Page 11 and 12: The above considerations are, of co
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- Page 17 and 18: and the initial state of our two-pa
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- Page 23 and 24: 2.3.3. Multi-terminal case We consi
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- Page 29: equilibrium and shot noise. For low
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- Page 39 and 40: and S" e A e< dE ¹(E )[1!¹
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- Page 47 and 48: we include weak localization e!ects
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- Page 59 and 60: Edge channels in the quantum Hall e
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- Page 69 and 70: Physically, this corresponds to ele
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- Page 73 and 74: Our starting point is Eq. (51), whi
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- Page 77 and 78: introducing the transmission coe$ci
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and the non-equilibrium resistance
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the sample. These electrons are des
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with D ,¹ (2!¹ ). Performing t
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For completeness, we mention that i
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We note here, however, that there i
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The noise power (201) is strongly v
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Fig. 32. Experimental results of Ku
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where Ya.M. Blanter, M. Bu( ttiker
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where the quantity is expressed th
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6.3. Interaction ewects Ya.M. Blant
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one "rst goes from the non-interact
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non-thermalized electrons, the high
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Fig. 34. Geometry of the chaotic ca
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which describes strictly ballistic
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approximately e/C. Between the peak
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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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