content_image/365030.jpg content_image/365040.jpg content_image/365037.jpg content_image/365039.jpg content_image/365038.jpg
<img src='content_image/365030.jpg'>

Though we can not exactly solve what y and z should be at K = 2 / 15 we can at least see 

<img src='content_image/365040.jpg'>

how y and z relate at this point. For an infinite 1-dimensional lattice we have that χ = e 2 $^{K}$, see e.g. $^{13}$. The second moment then should behave as 

Let ℓ = k − n/ 2 and σ = √ σ$_{2}$ . For high temperatures we expect ℓ/σ to be normally distributed and thus 

The probability ratio is then 

<img src='content_image/365037.jpg'>

<img src='content_image/365039.jpg'>

<img src='content_image/365038.jpg'>

