Spatial field correlation, the building block of mesoscopic fluctuations
arXiv:cond-mat/0112296 · doi:10.1103/PhysRevLett.88.123901
Abstract
The absence of self averaging in mesoscopic systems is a consequence of long-range intensity correlation. Microwave measurements suggest and diagrammatic calculations confirm that the correlation function of the normalized intensity with displacement of the source and detector, $ÎR$ and $Îr$, respectively, can be expressed as the sum of three terms, with distinctive spatial dependences. Each term involves only the sum or the product of the square of the field correlation function, $F \equiv F_{E}^2$. The leading-order term is the product, the next term is proportional to the sum. The third term is proportional to $[F(ÎR)F(Îr) + [F(ÎR)+F(Îr)] + 1]$.
Submitted to PRL