content_image/330174.jpg content_image/330176.jpg content_image/330177.jpg content_image/330182.jpg
have quite different behaviours, since their weak boson decays are different. The total e ± from fragmentations are described by the following functions 

<img src='content_image/330174.jpg'>

The type for all the Higgs bosons have the similar form, probably because they all are dominated by the H$_{d}$ components. For simplicity, we only present A$_{0}$ as follows 

<img src='content_image/330176.jpg'>

At last, the fitting functions for the neutralinos ˜ C 3 , 4 and charginos ˜ C 1 , 2 are given by C 0 3 : dN = exp 15 . 461 − 15 . 601 E 0 . 163 E 1 . 311 1 + 40 . 0 log(1 + 0 . 025 E ) 2 . 4 2 . 7 10 − 

<img src='content_image/330177.jpg'>

Basically, these fitting functions consist of three parts. The first part describes the low 

<img src='content_image/330182.jpg'>

energy region very well, the second logarithmic part is added to slow down the exceptional decreasing, and the last part is used to modulate the region near the DM mass cutoff region. This kind of fitting functions is not universal, and only applies to our parameter sets. We 

