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shot noise in mesoscopic conductors - Low Temperature Laboratory

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Our start<strong>in</strong>g po<strong>in</strong>t is Eq. (51), which <strong>in</strong> this form is given <strong>in</strong> Ref. [146]. Tak<strong>in</strong>g the scatter<strong>in</strong>g<br />

matrices to be energy <strong>in</strong>dependent, we write<br />

S(),S ()"<br />

e<br />

2 ¹ <br />

dE[ f (E, )#f (E, )]<br />

<br />

with the abbreviation<br />

Ya.M. Blanter, M. Bu( ttiker / Physics Reports 336 (2000) 1}166 73<br />

#<br />

<br />

¹ (1!¹ ) dE[ f (E, )#f (E, )] , (125)<br />

f (E, )"f (E)[1!f (E#)]#[1!f (E)] f (E#) . (126)<br />

Here the ¹ 's are, as before (energy <strong>in</strong>dependent) transmission coe$cients. Perform<strong>in</strong>g the<br />

<strong>in</strong>tegration, we obta<strong>in</strong><br />

S()" e<br />

22 coth <br />

2k ¹ <br />

#e<<br />

¹# (#e

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