shot noise in mesoscopic conductors - Low Temperature Laboratory

More documents

Recommendations

Info

60 Ya.M. Blanter, M. Bu( ttiker / Physics Reports 336 (2000) 1}166 Prior to the description of experimental results, we discuss brie#y a measurement of S on the quantum Hall conductor of Fig. 13. If current is incident from contact 4 (experiment A), or contact 2 (experiment B) alone we have for the current #uctuations at contact 3 S "S "(e
Fig. 19. (a) Geometry of a ring threaded by a #ux , demonstrating the Aharonov}Bohm e!ect in a weak magnetic "eld. (b) Conductance in units of e/2 (1) and shot noise power in units of e
Page 1 and 2:
Ya.M. Blanter, M. BuK ttiker / Phys
Page 3 and 4:
8. Concluding remarks, future prosp
Page 5 and 6:
text; they are usually extensions o
Page 7 and 8:
such reviews are not readily availa
Page 9 and 10: Ya.M. Blanter, M. Bu( ttiker / Phys
Page 11 and 12: The above considerations are, of co
Page 17 and 18: and the initial state of our two-pa
Page 23 and 24: 2.3.3. Multi-terminal case We consi
Page 25 and 26: Note that in the absence of time-de
Page 29 and 30: equilibrium and shot noise. For low
Page 39 and 40: and S" e A e< dE ¹(E )[1!¹
Page 41 and 42: arrier, situated in the region !w/2
Page 47 and 48: we include weak localization e!ects
Page 59: Edge channels in the quantum Hall e
Page 63 and 64: a manifestation of interference e!e
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
Page 85 and 86: and the non-equilibrium resistance
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
Page 111 and 112:
The noise power (201) is strongly v
Page 113 and 114:
Fig. 32. Experimental results of Ku
Page 115 and 116:
where Ya.M. Blanter, M. Bu( ttiker
Page 117 and 118:
where the quantity is expressed th
Page 119 and 120:
6.3. Interaction ewects Ya.M. Blant
Page 121 and 122:
Ya.M. Blanter, M. Bu( ttiker / Phys
Page 123 and 124:
one "rst goes from the non-interact
Page 125 and 126:
non-thermalized electrons, the high
Page 127 and 128:
Page 129 and 130:
Fig. 34. Geometry of the chaotic ca
Page 131 and 132:
Page 133 and 134:
which describes strictly ballistic
Page 135 and 136:
Page 137 and 138:
Page 139 and 140:
Page 141 and 142:
approximately e/C. Between the peak
Page 143 and 144:
Page 145 and 146:
Page 147 and 148:
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
Page 157 and 158:
Page 159 and 160:
Page 161 and 162:
Page 163 and 164:
Page 165 and 166:
show all

shot noise in mesoscopic conductors - Low Temperature Laboratory

Create successful ePaper yourself

Delete template?

Save as template?